Magnetic recording medium, magnetic recording and reproducing apparatus, magnetic tape cartridge, and magnetic tape cartridge group

ABSTRACT

In the magnetic recording medium, a number distribution A of a plurality of bright regions, based on equivalent circle diameters thereof, in a binarized image of a secondary electron image obtained by imaging a surface of the magnetic layer by a scanning electron microscope at an acceleration voltage of 5 kV and a number distribution B of a plurality of dark regions, based on equivalent circle diameters thereof, in a binarized image of a secondary electron image obtained by imaging a surface of the magnetic layer by a scanning electron microscope at an acceleration voltage of 2 kV respectively satisfy a predetermined number distribution.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority under 35 U.S.C 119 to Japanese PatentApplication No. 2020-010312 filed on Jan. 24, 2020. The aboveapplication is hereby expressly incorporated by reference, in itsentirety, into the present application.

BACKGROUND OF THE INVENTION 1. Field of the Invention

The present invention relates to a magnetic recording medium, a magneticrecording and reproducing apparatus, a magnetic tape cartridge, and amagnetic tape cartridge group.

2. Description of the Related Art

Recording of data on a magnetic recording medium and reproducing ofrecorded data are usually performed by causing a magnetic layer surfaceof the magnetic recording medium and a magnetic head (hereinafter,simply referred to as a “head”.) to come into contact with each other tobe slid on each other (for example, see JP2005-092967A).

SUMMARY OF THE INVENTION

Data recorded on various recording media such as a magnetic recordingmedium is called hot data, warm data, or cold data depending on anaccess frequency (reproduction frequency). The access frequencydecreases in the order of hot data, warm data, and cold data, and thecold data is usually stored in the recording medium while being recordedfor a long period of 10 years or more (for example, several decades).Recording and storing such cold data is called archiving (archive). Withdramatic increase in the amount of information and digitization ofvarious kinds of information in recent years, the amount of cold datarecorded and stored in the magnetic recording medium increases, andtherefore, attention is paid to a magnetic recording and reproducingsystem suitable for archiving.

Conventionally, in a test of a magnetic recording and reproducingapparatus (generally referred to as a “drive”.), since a usage form inwhich an access frequency is higher than that of an archive applicationwas assumed, usually, one magnetic recording medium was repeatedly slidwith respect to the same head without replacing the magnetic recordingmedium with a new one.

With respect to this, in recent years, a green tape test (GTT) has beenproposed as the test of the magnetic recording and reproducingapparatus. In the GTT, assuming a usage form specific to an archiveapplication in which cold data having a low access frequency is recordedand reproduced, a plurality (for example, several hundreds) of newmagnetic recording media are slid with respect to one head whilereplacing the magnetic recording medium.

As described above, the GTT is different from the test of theconventional magnetic recording and reproducing apparatus. Therefore, ina case where the GTT is adopted as the test of the magnetic recordingand reproducing apparatus, it is expected that a new performancedifferent from the conventional one is required for the magneticrecording medium. In this regard, the present inventor has consideredthat a magnetic recording medium that can contribute to obtaining afavorable reproduction quality in the GT will be desired in the future.A favorable reproduction quality in the GTT can be evaluated by, forexample, suppressing occurrence of reproduction errors in a case where aplurality of magnetic recording media are sequentially slid with respectto one head and data is read out from each magnetic recording medium inthe GTT under an environment of about room temperature. A magneticrecording medium capable of exhibiting such performance in the GTT,which is a test assuming a usage form specific to an archiveapplication, can be said to be a magnetic recording medium suitable foran archive recording medium.

In view of the above description, an object of an aspect of the presentinvention is to provide a magnetic recording medium suitable for anarchive recording medium, and more specifically, to provide a magneticrecording medium that can contribute to obtaining a favorablereproduction quality in a green tape test (GTT) under an environment ofabout room temperature.

An aspect of the present invention relates to a magnetic recordingmedium comprising:

-   -   a non-magnetic support; and    -   a magnetic layer including ferromagnetic powder,    -   in which a number distribution A of a plurality of bright        regions, based on equivalent circle diameters thereof, in a        binarized image of a secondary electron image obtained by        imaging a surface of the magnetic layer by a scanning electron        microscope at an acceleration voltage of 5 kV satisfies the        following (1) to (3):        -   (1) bright regions having an equivalent circle diameter of 1            nm or more and 50 nm or less are 10,000 or more and 30,000            or less;        -   (2) bright regions having an equivalent circle diameter of            51 nm or more and 100 nm or less are 7,000 or more and            25,000 or less; and        -   (3) bright regions having an equivalent circle diameter of            101 nm or more are 1,000 or more and 3,000 or less, and    -   a number distribution B of a plurality of dark regions, based on        equivalent circle diameters thereof, in a binarized image of a        secondary electron image obtained by imaging a surface of the        magnetic layer by a scanning electron microscope at an        acceleration voltage of 2 kV satisfies the following (4) to (6):        -   (4) dark regions having an equivalent circle diameter of 1            nm or more and 50 nm or less are 1,000 or more and 25,000 or            less;        -   (5) dark regions having an equivalent circle diameter of 51            nm or more and 100 nm or less are 200 or more and 5,000 or            less; and        -   (6) dark regions having an equivalent circle diameter of 101            nm or more are 0 or more and 200 or less.

In one embodiment, a total thickness of the magnetic recording mediummay be 5.3 μm or less.

In one embodiment, the magnetic recording medium may further comprise: anon-magnetic layer including non-magnetic powder between thenon-magnetic support and the magnetic layer.

In one embodiment, the magnetic recording medium may further comprise: aback coating layer including non-magnetic powder on a surface side ofthe non-magnetic support opposite to a surface side provided with themagnetic layer.

In one embodiment, the magnetic layer may include two or more types ofnon-magnetic powder.

In one embodiment, the non-magnetic powder of the magnetic layer mayinclude alumina powder.

In one embodiment, the non-magnetic powder of the magnetic layer mayinclude carbon black.

In one embodiment, the ferromagnetic powder may be hexagonal bariumferrite powder.

In one embodiment, the ferromagnetic powder may be hexagonal strontiumferrite powder.

In one embodiment, the ferromagnetic powder may be ε-iron oxide powder.

In one embodiment, a vertical squareness ratio of the magnetic recordingmedium may be 0.65 or more and 1.00 or less.

In one embodiment, a vertical coercive force of the magnetic recordingmedium is 2,500 Oe or more and 3,500 Oe or less.

In one embodiment, the magnetic recording medium may be a magnetic tape.

Another aspect of the present invention relates to a magnetic recordingand reproducing apparatus comprising the magnetic recording medium.

In one embodiment, the magnetic recording and reproducing apparatus mayfurther comprise: a magnetic head that has an inductive recordingelement having a first magnetic pole that generates a magnetic field anda second magnetic pole that is separated from the first magnetic polewith a write gap therebetween,

-   -   in which the first magnetic pole has a layer made of an alloy        containing Co and Fe as an outermost layer of a portion facing        the second magnetic pole with the write gap therebetween, and    -   the second magnetic pole has a layer made of an alloy containing        Co and Fe as an outermost layer of a portion facing the first        magnetic pole with the write gap therebetween.

In one embodiment, the magnetic recording and reproducing apparatus mayfurther comprise: a magnetic head having an inductive recording elementhaving a length of a write gap of 120 nm or less.

Still another aspect of the present invention relates to a magnetic tapecartridge comprising: the magnetic recording medium that is a magnetictape.

Still another aspect of the present invention relates to a magnetic tapecartridge group comprising: a plurality of the magnetic tape cartridges.

In one embodiment, in the magnetic tape cartridge group, in anenvironment of an atmosphere temperature of 21° C. and a relativehumidity of 50%, a slope α (hereinafter, referred to as a “GTT slopeα”.) of a signal-to-noise-ratio (SNR) with respect to the number ofrolls, the slope α being obtained by performing a reproduction test of atotal of 200 rolls of the magnetic tape cartridges using a singlemagnetic head, may be 0.5 dB/decade or less.

According to one aspect of the present invention, it is possible toprovide a magnetic recording medium suitable for an archive recordingmedium and a magnetic recording and reproducing apparatus including themagnetic recording medium. In addition, according to one aspect of thepresent invention, it is possible to provide a magnetic tape cartridgeand a magnetic tape cartridge group including the magnetic recordingmedium that is a magnetic tape.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a partially enlarged view of an example of a recordingelement.

FIG. 2 is a schematic cross-sectional view showing a configuration of awrite gap-side tip portion of the recording element shown in FIG. 1.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Magnetic Recording Medium

An aspect of the present invention relates to a magnetic recordingmedium including: a non-magnetic support; and a magnetic layer includingferromagnetic powder, in which a number distribution A of a plurality ofbright regions, based on equivalent circle diameters thereof, in abinarized image of a secondary electron image obtained by imaging asurface of the magnetic layer by a scanning electron microscope at anacceleration voltage of 5 kV satisfies the above-described (1) to (3),and a number distribution B of a plurality of dark regions, based onequivalent circle diameters thereof, in a binarized image of a secondaryelectron image obtained by imaging a surface of the magnetic layer by ascanning electron microscope at an acceleration voltage of 2 kVsatisfies the above-described (4) to (6).

The present inventor has conducted extensive studies in order to obtaina magnetic recording medium capable of exhibiting the above-describedperformance, which is considered to be required in the future, and hasconsidered that a value of the GTT slope α, which will be described indetail below, may correlate with a reproduction quality in a green tapetest (GTT) under an environment of about room temperature. As a resultof further intensive studies based on such knowledge, the numberdistribution A and the number distribution B of a state of a magneticlayer surface of the magnetic recording medium are controlled asdescribed above. According to such a magnetic recording medium, it ispossible to obtain a favorable reproduction quality in a green tape test(GTT) under an environment of about room temperature.

Hereinafter, the magnetic recording medium will be described morespecifically.

A scanning electron microscope used for obtaining the numberdistribution A and the number distribution B in the present inventionand the present specification is a field emission-scanning electronmicroscope (FE-SEM). As the FE-SEM, for example, FE-SEM S4800manufactured by Hitachi, Ltd. can be used, and this FE-SEM was used inExamples described below.

In a case where the number distribution A and the number distribution Bare respectively obtained, the magnetic layer surface is not coatedbefore an SEM image is captured.

Each imaging is performed by selecting a non-imaging region on themagnetic layer surface.

The SEM image to be captured is a secondary electron image.

The equivalent circle diameter may be obtained in 1 nm increments byrounding off the first decimal point and rounding down the seconddecimal point.

In a case where the number distribution A is obtained, in themeasurement of the number of bright regions, a bright region where onlya part is included in the binarized image and the remaining part isoutside the binarized image is excluded from the measurement object.

In addition, in a case where the number distribution B is obtained, inthe measurement of the number of dark regions, a dark region where onlya part is included in the binarized image and the remaining part isoutside the binarized image is excluded from the measurement object.

In the present invention and the present specification, the “magneticlayer surface (surface of the magnetic layer)” has the same meaning as asurface of the magnetic recording medium on a magnetic layer side.

Measurement Method of Number Distribution

Measurement Method of Number Distribution A

In the present invention and the present specification, the “numberdistribution A” is a number distribution measured by the followingmethod.

A secondary electron image of the magnetic layer surface of the magneticrecording medium to be measured is captured using a scanning electronmicroscope (FE-SEM). As imaging conditions, an acceleration voltage is 5kV, an operating distance is 5 mm, and an imaging magnification is10,000. In imaging, a non-imaging region on the magnetic layer surfaceis selected, focus adjustment is performed under the imaging conditions,and a secondary electron image is captured. A part (micron bar, crossmark, or the like) for displaying the size and the like is erased fromthe captured image, and a secondary electron image having the number ofpixels of 960 pixels×1280 pixels is acquired.

The above operation is performed 100 times at different positions on themagnetic layer surface of the magnetic recording medium to be measured.

The secondary electron image thus acquired is taken into imageprocessing software, and is binarized by the following procedure. Asimage analysis software, for example, free software ImageJ can be used.The image is divided into a bright region (white part) and a dark region(black part) by binarization processing.

For a threshold value for binarizing the secondary electron imageacquired above, a lower limit is set to 210 gradations and an upperlimit is set to 255 gradations, and the binarization processing isexecuted based on these two threshold values. After the binarizationprocessing, noise component removal processing is performed by the imageanalysis software. The noise component removal processing can beperformed by the following method, for example. In the image analysissoftware ImageJ, noise cut processing Despeckle is selected to removethe noise component.

For the binarized image thus obtained, the number of bright regions(that is, white parts) and the area of each bright region are obtainedby the image analysis software. From the area of the bright regionobtained here, the equivalent circle diameter of each bright region isobtained. Specifically, an equivalent circle diameter L is calculatedfrom the obtained area A by (A/π){circumflex over ( )}(½)×2=L. Here, theoperator “{circumflex over ( )}” represents a power.

The above processes are performed on the binarized image (100 images)obtained above.

In this manner, the number distribution A is obtained.

Measurement Method of Number Distribution B

In the present invention and the present specification, the “numberdistribution B” is a number distribution measured by the followingmethod.

A secondary electron image of the magnetic layer surface of the magneticrecording medium to be measured is captured using a scanning electronmicroscope (FE-SEM). As imaging conditions, an acceleration voltage is 2kV, an operating distance is 5 mm, and an imaging magnification is10,000. In imaging, a non-imaging region on the magnetic layer surfaceis selected, focus adjustment is performed under the imaging conditions,and a secondary electron image is captured. A part (micron bar, crossmark, or the like) for displaying the size and the like is erased fromthe captured image, and a secondary electron image having the number ofpixels of 960 pixels×1280 pixels is acquired.

The above operation is performed 100 times at different positions on themagnetic layer surface of the magnetic recording medium to be measured.

The secondary electron image thus acquired is taken into imageprocessing software, and is binarized by the following procedure. Asimage analysis software, for example, free software ImageJ can be used.

For a threshold value for binarizing the secondary electron imageacquired above, a lower limit is set to 0 gradation and an upper limitis set to 75 gradations, and the binarization processing is executedbased on these two threshold values. After the binarization processing,noise component removal processing is performed by the image analysissoftware. The noise component removal processing can be performed by thefollowing method, for example. In the image analysis software ImageJ,noise cut processing Despeckle is selected to remove the noisecomponent.

In the binarized image thus obtained, the number of dark regions (thatis, black parts) and the area of each dark region are obtained by theimage analysis software. From the area of the dark region obtained here,the equivalent circle diameter of each dark region is obtained.Specifically, an equivalent circle diameter L is calculated from theobtained area A by (A/π){circumflex over ( )}(½)×2=L.

The above processes are performed on the binarized image (100 images)obtained above. In this manner, the number distribution B is obtained.

Number Distribution A and Number Distribution B

In the magnetic recording medium, the number distribution A obtained bythe above-described method satisfies the following (1) to (3):

-   -   (1) bright regions having an equivalent circle diameter of 1 nm        or more and 50 nm or less are 10,000 or more and 30,000 or less;    -   (2) bright regions having an equivalent circle diameter of 51 nm        or more and 100 nm or less are 7,000 or more and 25,000 or less;        and    -   (3) bright regions having an equivalent circle diameter of 101        nm or more are 1,000 or more and 3,000 or less.

Further, in the magnetic recording medium, the number distribution Bobtained by the above-described method satisfies the following (4) to(6):

-   -   (4) dark regions having an equivalent circle diameter of 1 nm or        more and 50 nm or less are 1,000 or more and 25,000 or less;    -   (5) dark regions having an equivalent circle diameter of 51 nm        or more and 100 nm or less are 200 or more and 5,000 or less;        and    -   (6) dark regions having an equivalent circle diameter of 101 nm        or more are 0 or more and 200 or less.

The magnetic layer is usually formed by using a magnetic layer formingcomposition containing at least one kind of non-magnetic powder inaddition to ferromagnetic powder. For the number distribution A and thenumber distribution B obtained by the above-described method, thepresent inventor considers that the number distribution A can be anindex of an existence state of the non-magnetic powder (hereinafter,referred to as an “abrasive”.) included in the magnetic layer on themagnetic layer surface in order to impart abradability to the magneticlayer surface. Further, the present inventor considers that the numberdistribution B can be an index of an existence state of the non-magneticpowder (hereinafter, referred to as a “filler”.) included in themagnetic layer on the magnetic layer surface in order to formappropriate protrusions on the magnetic layer surface for controllingfriction characteristics. The present inventor supposes that, bycontrolling the number distribution A and the number distribution B asdescribed above, inhibition of the scrape of the head, the scrape of themagnetic recording medium, and/or the adhesion of foreign mattergenerated by some cause to the head in a GTT under an environment ofabout room temperature can contribute to obtaining a favorablereproduction quality in a GTT under an environment of about roomtemperature. The environment of about room temperature may be, forexample, an environment of an atmosphere temperature of about 18° C. to27° C. A humidity of the environment may be, for example, about 40% to60% as a relative humidity.

Regarding the above (1), the number of bright regions having anequivalent circle diameter of 1 nm or more and 50 nm or less is 10,000or more and 30,000 or less. From the viewpoint of cleanability, thenumber of such bright regions is preferably 15,000 or more, and morepreferably 20,000 or more. In addition, from the viewpoint of surfaceproperty, the number of such bright regions is preferably 28,000 orless, and more preferably 25,000 or less.

Regarding the above (2), the number of bright regions having anequivalent circle diameter of 51 nm or more and 100 nm or less is 7.000or more and 25,000 or less. From the viewpoint of cleanability, thenumber of such bright regions is preferably 8,000 or more, and morepreferably 9,000 or more. In addition, from the viewpoint of surfaceproperty, the number of such bright regions is preferably 24,000 orless, and more preferably 23,000 or less.

Regarding the above (3), the number of bright regions having anequivalent circle diameter of 101 nm or more is 1,000 or more and 3,000or less. From the viewpoint of cleanability, the number of such brightregions is preferably 1,500 or more, and more preferably 2,000 or more.In addition, from the viewpoint of surface property, the number of suchbright regions is preferably 2,800 or less, and more preferably 2,500 orless. In an aspect, the number of the bright regions may be less than3,000. In addition, in an aspect, the number of the bright regions maybe more than 1,000.

Regarding the above (4), the number of dark regions having an equivalentcircle diameter of 1 nm or more and 50 nm or less is 1,000 or more and25,000 or less. From the viewpoint of friction characteristics, thenumber of such dark regions is preferably 2,000 or more, and morepreferably 3,000 or more. In addition, from the viewpoint ofcleanability, the number of such dark regions is preferably 23,000 orless, and more preferably 20,000 or less. In an aspect, the number ofthe dark regions may be more than 1,000.

Regarding the above (5), the number of dark regions having an equivalentcircle diameter of 51 nm or more and 100 nm or less is 200 or more and5,000 or less. From the viewpoint of friction characteristics, thenumber of such dark regions is preferably 250 or more, and morepreferably 300 or more. In addition, from the viewpoint of cleanability,the number of such dark regions is preferably 4,500 or less, and morepreferably 4,000 or less.

Regarding the above (6), the number of dark regions having an equivalentcircle diameter of 101 nm or more is 0 or more and 200 or less. From theviewpoint of friction characteristics, the number of such dark regionsis preferably 10 or more, and more preferably 20 or more. In addition,from the viewpoint of cleanability, the number of such dark regions ispreferably 180 or less, and more preferably 150 or less. In an aspect,the number of the dark regions may be less than 200.

The number distribution A and the number distribution B are controlledby the kind of components to be added to the magnetic layer formingcomposition used for forming the magnetic layer and a method forpreparing such composition (for example, a dispersion method, aclassification method, or the like). For specific examples of thecontrol method, Examples described below can be referred to.

Hereinafter, the magnetic recording medium will be described morespecifically.

Magnetic Layer

Ferromagnetic Powder

As the ferromagnetic powder included in the magnetic layer, well-knownferromagnetic powder as ferromagnetic powder used in magnetic layers ofvarious magnetic recording media can be used alone or in combination oftwo or more. From the viewpoint of improving recording density, it ispreferable to use ferromagnetic powder having a small average particlesize. From this point, the average particle size of ferromagnetic powderis preferably 50 nm or less, more preferably 45 nm or less, still morepreferably 40 nm or less, still more preferably 35 nm or less, stillmore preferably 30 nm or less, still more preferably 25 nm or less, andstill more preferably 20 nm or less. On the other hand, from a viewpointof magnetization stability, the average particle size of ferromagneticpowder is preferably 5 nm or more, more preferably 8 nm or more, stillmore preferably 10 nm or more, still more preferably 15 nm or more, andstill more preferably 20 nm or more.

Hexagonal Ferrite Powder Preferred specific examples of theferromagnetic powder include hexagonal ferrite powder. For details ofthe hexagonal ferrite powder, for example, descriptions disclosed inparagraphs 0012 to 0030 of JP2011-225417A, paragraphs 0134 to 0136 ofJP2011-216149A, paragraphs 0013 to 0030 of JP2012-204726A, andparagraphs 0029 to 0084 of JP2015-127985A can be referred to.

In the present invention and the present specification, “hexagonalferrite powder” refers to ferromagnetic powder in which a hexagonalferrite type crystal structure is detected as a main phase by X-raydiffraction analysis. The main phase refers to a structure to which thehighest intensity diffraction peak in an X-ray diffraction spectrumobtained by X-ray diffraction analysis is attributed. For example, in acase where the highest intensity diffraction peak is attributed to ahexagonal ferrite type crystal structure in an X-ray diffractionspectrum obtained by X-ray diffraction analysis, it is determined thatthe hexagonal ferrite type crystal structure is detected as the mainphase. In a case where only a single structure is detected by X-raydiffraction analysis, this detected structure is taken as the mainphase. The hexagonal ferrite type crystal structure includes at least aniron atom, a divalent metal atom and an oxygen atom, as a constituentatom. The divalent metal atom is a metal atom that can be a divalentcation as an ion, and examples thereof may include an alkaline earthmetal atom such as a strontium atom, a barium atom, and a calcium atom,a lead atom, and the like. In the present invention and the presentspecification, hexagonal strontium ferrite powder means that the maindivalent metal atom included in this powder is a strontium atom, andhexagonal barium ferrite powder means that the main divalent metal atomincluded in this powder is a barium atom. The main divalent metal atomrefers to a divalent metal atom that accounts for the most on an at %basis among divalent metal atoms included in the powder. Here, a rareearth atom is not included in the above divalent metal atom. The “rareearth atom” in the present invention and the present specification isselected from the group consisting of a scandium atom (Sc), an yttriumatom (Y), and a lanthanoid atom. The Lanthanoid atom is selected fromthe group consisting of a lanthanum atom (La), a cerium atom (Ce), apraseodymium atom (Pr), a neodymium atom (Nd), a promethium atom (Pm), asamarium atom (Sm), a europium atom (Eu), a gadolinium atom (Gd), aterbium atom (Tb), a dysprosium atom (Dy), a holmium atom (Ho), anerbium atom (Er), a thulium atom (Tm), an ytterbium atom (Yb), and alutetium atom (Lu).

Hereinafter, the hexagonal strontium ferrite powder, which is an aspectof the hexagonal ferrite powder, will be described in more detail.

An activation volume of hexagonal strontium ferrite powder is preferablyin a range of 800 to 1600 nm³. The finely granulated hexagonal strontiumferrite powder having an activation volume in the above range issuitable for manufacturing a magnetic recording medium exhibitingexcellent electromagnetic conversion characteristics. The activationvolume of the hexagonal strontium ferrite powder is preferably 800 nm³or more, for example, 850 nm³ or more. Further, from the viewpoint offurther improving the electromagnetic conversion characteristics, theactivation volume of the hexagonal strontium ferrite powder is morepreferably 1500 nm³ or less, still more preferably 1400 nm³ or less,still more preferably 1300 nm³ or less, still more preferably 1200 nm³or less, and still more preferably 1100 nm³ or less. The same applies toan activation volume of the hexagonal barium ferrite powder.

The “activation volume” is a unit of magnetization reversal and is anindex indicating the magnetic size of a particle. An activation volumedescribed in the present invention and the present specification and ananisotropy constant Ku which will be described below are values obtainedfrom the following relational expression between a coercive force He andan activation volume V, by performing measurement in an Hc measurementportion at a magnetic field sweep rate of 3 minutes and 30 minutes usinga vibrating sample magnetometer (measurement temperature: 23° C.±1° C.).For a unit of the anisotropy constant Ku, 1 erg/cc=1.0×10⁻¹ J/m³.Hc=2Ku/Ms{1−[(kT/KuV)ln(At/0.693)]^(1/2)}

[In the above formula, Ku: anisotropy constant (unit: J/m³), Ms:saturation magnetization (Unit: kA/m), k: Boltzmann constant, T:absolute temperature (unit: K), V: activation volume (unit: cm³), A:spin precession frequency (unit: s⁻¹), t: magnetic field reversal time(unit: s)]

An index for reducing thermal fluctuation, in other words, improvingthermal stability may include an anisotropy constant Ku. The hexagonalstrontium ferrite powder preferably has Ku of 1.8×10⁵ J/m³ or more, andmore preferably has Ku of 2.0×10⁵ J/m³ or more. Ku of the hexagonalstrontium ferrite powder may be, for example, 2.5×10⁵ J/m³ or less.Here, it means that the higher Ku is, the higher thermal stability is,this is preferable, and thus, a value thereof is not limited to thevalues exemplified above.

The hexagonal strontium ferrite powder may or may not include a rareearth atom. In a case where the hexagonal strontium ferrite powderincludes a rare earth atom, it is preferable to include a rare earthatom at a content (bulk content) of 0.5 to 5.0 at % with respect to 100at % of an iron atom. In an aspect, the hexagonal strontium ferritepowder including a rare earth atom may have a rare earth atom surfacelayer portion uneven distribution property. In the present invention andthe present specification, the “rare earth atom surface layer portionuneven distribution property” means that a rare earth atom content withrespect to 100 at % of an iron atom in a solution obtained by partiallydissolving hexagonal strontium ferrite powder with an acid (hereinafter,referred to as a “rare earth atom surface layer portion content” orsimply a “surface layer portion content” for a rare earth atom.) and arare earth atom content with respect to 100 at % of an iron atom in asolution obtained by totally dissolving hexagonal strontium ferritepowder with an acid (hereinafter, referred to as a “rare earth atom bulkcontent” or simply a “bulk content” for a rare earth atom.) satisfy aratio of a rare earth atom surface layer portion content/a rare earthatom bulk content >1.0. A rare earth atom content in hexagonal strontiumferrite powder which will be described below is the same meaning as therare earth atom bulk content. On the other hand, partial dissolutionusing an acid dissolves a surface layer portion of a particleconfiguring hexagonal strontium ferrite powder, and thus, a rare earthatom content in a solution obtained by partial dissolution is a rareearth atom content in a surface layer portion of a particle configuringhexagonal strontium ferrite powder. A rare earth atom surface layerportion content satisfying a ratio of “rare earth atom surface layerportion content/rare earth atom bulk content >1.0” means that in aparticle of hexagonal strontium ferrite powder, rare earth atoms areunevenly distributed in a surface layer portion (that is, more than aninside). The surface layer portion in the present invention and thepresent specification means a partial region from a surface of aparticle configuring hexagonal strontium ferrite powder toward aninside.

In a case where hexagonal strontium ferrite powder includes a rare earthatom, a rare earth atom content (bulk content) is preferably in a rangeof 0.5 to 5.0 at % with respect to 100 at % of an iron atom. It isconsidered that a bulk content in the above range of the included rareearth atom and uneven distribution of the rare earth atoms in a surfacelayer portion of a particle configuring hexagonal strontium ferritepowder contribute to suppression of a decrease in reproduction output inrepeated reproduction. It is supposed that this is because hexagonalstrontium ferrite powder includes a rare earth atom with a bulk contentin the above range, and rare earth atoms are unevenly distributed in asurface layer portion of a particle configuring hexagonal strontiumferrite powder, and thus it is possible to increase an anisotropyconstant Ku. The higher a value of an anisotropy constant Ku is, themore a phenomenon called so-called thermal fluctuation can be suppressed(in other words, thermal stability can be improved). By suppressingoccurrence of thermal fluctuation, it is possible to suppress a decreasein reproduction output during repeated reproduction. It is supposed thatuneven distribution of rare earth atoms in a particulate surface layerportion of hexagonal strontium ferrite powder contributes tostabilization of spins of iron (Fe) sites in a crystal lattice of asurface layer portion, and thus, an anisotropy constant Ku may beincreased.

Moreover, it is supposed that the use of hexagonal strontium ferritepowder having a rare earth atom surface layer portion unevendistribution property as ferromagnetic powder in the magnetic layer alsocontributes to inhibition of a magnetic layer surface from being scrapedby being slid with respect to the magnetic head. That is, it is supposedthat hexagonal strontium ferrite powder having rare earth atom surfacelayer portion uneven distribution property can also contribute to theimprovement of running durability of the magnetic recording medium. Itis supposed that this may be because uneven distribution of rare earthatoms on a surface of a particle configuring hexagonal strontium ferritepowder contributes to the improvement of interaction between theparticle surface and an organic substance (for example, a binding agentand/or an additive) included in the magnetic layer, and, as a result, astrength of the magnetic layer is improved.

From the viewpoint of further suppressing a decrease in reproductionoutput during repeated reproduction and/or the viewpoint of furtherimproving the running durability, the rare earth atom content (bulkcontent) is more preferably in a range of 0.5 to 4.5 at %, still morepreferably in a range of 1.0 to 4.5 at %, and still more preferably in arange of 1.5 to 4.5 at %.

The bulk content is a content obtained by totally dissolving hexagonalstrontium ferrite powder. In the present invention and the presentspecification, unless otherwise noted, the content of an atom means abulk content obtained by totally dissolving hexagonal strontium ferritepowder. The hexagonal strontium ferrite powder including a rare earthatom may include only one kind of rare earth atom as the rare earthatom, or may include two or more kinds of rare earth atoms. The bulkcontent in the case of including two or more types of rare earth atomsis obtained for the total of two or more types of rare earth atoms. Thisalso applies to other components in the present invention and thepresent specification. That is, unless otherwise noted, a certaincomponent may be used alone or in combination of two or more. A contentamount or a content in a case where two or more components are usedrefers to that for the total of two or more components.

In a case where the hexagonal strontium ferrite powder includes a rareearth atom, the included rare earth atom may be any one or more of rareearth atoms. As a rare earth atom that is preferable from the viewpointof further suppressing a decrease in reproduction output in repeatedreproduction, there are a neodymium atom, a samarium atom, a yttriumatom, and a dysprosium atom, here, the neodymium atom, the samariumatom, and the yttrium atom are more preferable, and a neodymium atom isstill more preferable.

In the hexagonal strontium ferrite powder having a rare earth atomsurface layer portion uneven distribution property, the rare earth atomsmay be unevenly distributed in the surface layer portion of a particleconfiguring the hexagonal strontium ferrite powder, and the degree ofuneven distribution is not limited. For example, for a hexagonalstrontium ferrite powder having a rare earth atom surface layer portionuneven distribution property, a ratio between a surface layer portioncontent of a rare earth atom obtained by partial dissolution underdissolution conditions which will be described below and a bulk contentof a rare earth atom obtained by total dissolution under dissolutionconditions which will be described below, that is, “surface layerportion content/bulk content” exceeds 1.0 and may be 1.5 or more.“Surface layer portion content/bulk content” larger than 1.0 means thatin a particle configuring the hexagonal strontium ferrite powder, rareearth atoms are unevenly distributed in the surface layer portion (thatis, more than in the inside). Further, a ratio between a surface layerportion content of a rare earth atom obtained by partial dissolutionunder dissolution conditions which will be described below and a bulkcontent of a rare earth atom obtained by total dissolution under thedissolution conditions which will be described below, that is, “surfacelayer portion content/bulk content” may be, for example, 10.0 or less,9.0 or less, 8.0 or less, 7.0 or less, 6.0 or less, 5.0 or less, or 4.0or less. Here, in the hexagonal strontium ferrite powder having a rareearth atom surface layer portion uneven distribution property, the rareearth atoms may be unevenly distributed in the surface layer portion ofa particle configuring the hexagonal strontium ferrite powder, and“surface layer portion content/bulk content” is not limited to theexemplified upper limit or lower limit.

The partial dissolution and the total dissolution of the hexagonalstrontium ferrite powder will be described below. For the hexagonalstrontium ferrite powder that exists as a powder, the partially andtotally dissolved sample powder is taken from the same lot of powder. Onthe other hand, for the hexagonal strontium ferrite powder included inthe magnetic layer of the magnetic recording medium, a part of thehexagonal strontium ferrite powder taken out from the magnetic layer issubjected to partial dissolution, and the other part is subjected tototal dissolution. The hexagonal strontium ferrite powder can be takenout from the magnetic layer by a method described in a paragraph 0032 ofJP2015-091747A, for example.

The partial dissolution means that dissolution is performed such that,at the end of dissolution, the residue of the hexagonal strontiumferrite powder can be visually checked in the solution. For example, bypartial dissolution, it is possible to dissolve a region of 10 to 20mass % of the particle configuring the hexagonal strontium ferritepowder with the total particle being 100 mass %. On the other hand, thetotal dissolution means that dissolution is performed such that, at theend of dissolution, the residue of the hexagonal strontium ferritepowder cannot be visually checked in the solution.

The partial dissolution and measurement of the surface layer portioncontent are performed by the following method, for example. Here, thefollowing dissolution conditions such as an amount of sample powder areexamples, and dissolution conditions for partial dissolution and totaldissolution can be employed in any manner.

A container (for example, a beaker) containing 12 mg of sample powderand 10 mL of 1 mol/L hydrochloric acid is held on a hot plate at a settemperature of 70° C. for 1 hour. The obtained solution is filtered by amembrane filter of 0.1 μm. Elemental analysis of the filtrated solutionis performed by an inductively coupled plasma (ICP) analyzer. In thisway, the surface layer portion content of a rare earth atom with respectto 100 at % of an iron atom can be obtained. In a case where a pluralityof types of rare earth atoms are detected by elemental analysis, thetotal content of all rare earth atoms is defined as the surface layerportion content. This also applies to the measurement of the bulkcontent.

On the other hand, the total dissolution and measurement of the bulkcontent are performed by the following method, for example.

A container (for example, a beaker) containing 12 mg of sample powderand 10 mL of 4 mol/L hydrochloric acid is held on a hot plate at a settemperature of 80° C. for 3 hours. Thereafter, the method is carried outin the same manner as the partial dissolution and the measurement of thesurface layer portion content, and the bulk content with respect to 100at % of an iron atom can be obtained.

From the viewpoint of increasing the reproduction output in a case ofreproducing data recorded on the magnetic recording medium, it isdesirable that mass magnetization as of the ferromagnetic powderincluded in the magnetic recording medium is high. In this regard, thehexagonal strontium ferrite powder including a rare earth atom but nothaving the rare earth atom surface layer portion uneven distributionproperty tends to have as largely lower than the hexagonal strontiumferrite powder including no rare earth atom. On the other hand, it isconsidered that hexagonal strontium ferrite powder having a rare earthatom surface layer portion uneven distribution property is preferable insuppressing such a large decrease in σs. In an aspect, as of thehexagonal strontium ferrite powder may be 45 A·m²/kg or more, and may be47 A·m²/kg or more. On the other hand, from the viewpoint of noisereduction, as is preferably 80 A·m²/kg or less and more preferably 60A·m²/kg or less, as can be measured using a well-known measuring device,such as a vibrating sample magnetometer, capable of measuring magneticproperties. In the present invention and the present specification,unless otherwise noted, the mass magnetization as is a value measured ata magnetic field intensity of 15 kOe. 1 [kOe]=10⁶/4π [A/m]

Regarding the content (bulk content) of a constituent atom of thehexagonal strontium ferrite powder, a strontium atom content may be, forexample, in a range of 2.0 to 15.0 at % with respect to 100 at % of aniron atom. In an aspect, in the hexagonal strontium ferrite powder, adivalent metal atom included in the powder may be only a strontium atom.In another aspect, the hexagonal strontium ferrite powder may includeone or more other divalent metal atoms in addition to a strontium atom.For example, a barium atom and/or a calcium atom may be included. In acase where another divalent metal atom other than a strontium atom isincluded, a barium atom content and a calcium atom content in thehexagonal strontium ferrite powder are, for example, in a range of 0.05to 5.0 at % with respect to 100 at % of an iron atom, respectively.

As a crystal structure of hexagonal ferrite, a magnetoplumbite type(also referred to as an “M type”.), a W type, a Y type, and a Z type areknown. The hexagonal strontium ferrite powder may have any crystalstructure. The crystal structure can be checked by X-ray diffractionanalysis. In the hexagonal strontium ferrite powder, a single crystalstructure or two or more crystal structures may be detected by X-raydiffraction analysis. For example, according to an aspect, in thehexagonal strontium ferrite powder, only the M-type crystal structuremay be detected by X-ray diffraction analysis. For example, M-typehexagonal ferrite is represented by a composition formula of AFe₁₂O₁₉.Here, A represents a divalent metal atom, and in a case where thehexagonal strontium ferrite powder is the M-type, A is only a strontiumatom (Sr), or in a case where, as A, a plurality of divalent metal atomsare included, as described above, a strontium atom (Sr) accounts for themost on an at % basis. The divalent metal atom content of the hexagonalstrontium ferrite powder is usually determined by the type of crystalstructure of the hexagonal ferrite and is not particularly limited. Thesame applies to the iron atom content and the oxygen atom content. Thehexagonal strontium ferrite powder may include at least an iron atom, astrontium atom, and an oxygen atom, and may further include a rare earthatom. Furthermore, the hexagonal strontium ferrite powder may or may notinclude atoms other than these atoms. As an example, the hexagonalstrontium ferrite powder may include an aluminum atom (Al). A content ofan aluminum atom can be, for example, 0.5 to 10.0 at % with respect to100 at % of an iron atom. From the viewpoint of further suppressing adecrease in reproduction output in repeated reproduction, the hexagonalstrontium ferrite powder includes an iron atom, a strontium atom, anoxygen atom, and a rare earth atom, and the content of atoms other thanthese atoms is preferably 10.0 at % or less, more preferably in a rangeof 0 to 5.0 at %, and may be 0 at % with respect to 100 at % of an ironatom. That is, in an aspect, the hexagonal strontium ferrite powder maynot include atoms other than an iron atom, a strontium atom, an oxygenatom, and a rare earth atom. The content expressed in at % is obtainedby converting a content of each atom (unit: mass %) obtained by totallydissolving hexagonal strontium ferrite powder into a value expressed inat % using an atomic weight of each atom. Further, in the presentinvention and the present specification, “not include” for a certainatom means that a content measured by an ICP analyzer after totaldissolution is 0 mass %. A detection limit of the ICP analyzer isusually 0.01 parts per million (ppm) or less on a mass basis. The “notincluded” is used as a meaning including that an atom is included in anamount less than the detection limit of the ICP analyzer. In an aspect,the hexagonal strontium ferrite powder may not include a bismuth atom(Bi).

Metal Powder

Preferable specific examples of the ferromagnetic powder includeferromagnetic metal powder. For details of the ferromagnetic metalpowder, for example, descriptions disclosed in paragraphs 0137 to 0141of JP2011-216149A and paragraphs 0009 to 0023 of JP2005-251351A can bereferred to.

ε-Iron Oxide Powder

Preferable specific examples of the ferromagnetic powder include ε-ironoxide powder. In the present invention and the present specification,“ε-iron oxide powder” refers to ferromagnetic powder in which an ε-ironoxide type crystal structure is detected as a main phase by X-raydiffraction analysis. For example, in a case where the highest intensitydiffraction peak is attributed to an ε-iron oxide type crystal structurein an X-ray diffraction spectrum obtained by X-ray diffraction analysis,it is determined that the ε-iron oxide type crystal structure isdetected as the main phase. As a manufacturing method of the ε-ironoxide powder, a manufacturing method from a goethite, a reverse micellemethod, and the like are known. All of the manufacturing methods arewell known. Regarding a method of manufacturing ε-iron oxide powder inwhich a part of Fe is substituted with substitutional atoms such as Ga,Co, Ti, Al, or Rh, a description disclosed in J. Jpn. Soc. PowderMetallurgy Vol. 61 Supplement, No. S1, pp. S280 to S284, J. Mater. Chem.C, 2013, 1, pp. 5200 to 5206 can be referred to, for example. Here, themanufacturing method of ε-iron oxide powder capable of being used as theferromagnetic powder in the magnetic layer of the magnetic recordingmedium is not limited to the methods described here.

An activation volume of the ε-iron oxide powder is preferably in a rangeof 300 to 1500 nm³. The finely granulated ε-iron oxide powder having anactivation volume in the above range is suitable for manufacturing amagnetic recording medium exhibiting excellent electromagneticconversion characteristics. The activation volume of the ε-iron oxidepowder is preferably 300 nm³ or more, for example, 500 nm³ or more.Further, from the viewpoint of further improving the electromagneticconversion characteristics, the activation volume of the ε-iron oxidepowder is more preferably 1400 nm³ or less, still more preferably 1300nm³ or less, still more preferably 1200 nm³ or less, and still morepreferably 1100 nm³ or less.

An index for reducing thermal fluctuation, in other words, improvingthermal stability may include an anisotropy constant Ku. The ε-ironoxide powder preferably has Ku of 3.0×10⁴ J/m³ or more, and morepreferably has Ku of 8.0×10⁴ J/m³ or more. Ku of the ε-iron oxide powdermay be, for example, 3.0×10⁵ J/m³ or less. Here, it means that thehigher Ku is, the higher thermal stability is, this is preferable, andthus, a value thereof is not limited to the values exemplified above.

From the viewpoint of increasing the reproduction output in a case ofreproducing data recorded on the magnetic recording medium, it isdesirable that mass magnetization as of the ferromagnetic powderincluded in the magnetic recording medium is high. In this regard, in anaspect, as of the ε-iron oxide powder may be 8 A·m²/kg or more, and maybe 12 A·m²/kg or more. On the other hand, from the viewpoint of noisereduction, as of the ε-iron oxide powder is preferably 40 A·m²/kg orless and more preferably 35 A·m²/kg or less.

In the present invention and the present specification, unless otherwisenoted, an average particle size of various types of powder such asferromagnetic powder is a value measured by the following method using atransmission electron microscope.

The powder is imaged at an imaging magnification of 100,000 using atransmission electron microscope, and the image is printed on printingpaper so that the total magnification ratio is 500,000 to obtain animage of particles configuring the powder. A target particle is selectedfrom the obtained image of particles, an outline of the particle istraced with a digitizer, and a size of the particle (primary particle)is measured. The primary particle is an independent particle which isnot aggregated.

The measurement described above is performed regarding 500 particlesrandomly extracted. An arithmetic average of the particle sizes of 500particles obtained as described above is an average particle size of thepowder. As the transmission electron microscope, a transmission electronmicroscope H-9000 manufactured by Hitachi, Ltd. can be used, forexample. In addition, the measurement of the particle size can beperformed by well-known image analysis software, for example, imageanalysis software KS-400 manufactured by Carl Zeiss. An average particlesize shown in Examples which will be described below is a value measuredby using a transmission electron microscope H-9000 manufactured byHitachi, Ltd. as the transmission electron microscope, and imageanalysis software KS-400 manufactured by Carl Zeiss as the imageanalysis software, unless otherwise noted. In the present invention andthe present specification, the powder means an aggregate of a pluralityof particles. For example, ferromagnetic powder means an aggregate of aplurality of ferromagnetic particles. Further, the aggregate of theplurality of particles not only includes an aspect in which particlesconfiguring the aggregate directly come into contact with each other,but also includes an aspect in which a binding agent or an additivewhich will be described below is interposed between the particles. Theterm “particle” is used to describe powder in some cases.

As a method of taking sample powder from the magnetic recording mediumin order to measure the particle size, a method disclosed in a paragraph0015 of JP2011-048878A can be used, for example.

In the present invention and the present specification, unless otherwisenoted, (1) in a case where the shape of the particle observed in theparticle image described above is a needle shape, a fusiform shape, or acolumnar shape (here, a height is greater than a maximum long diameterof a bottom surface), the size (particle size) of the particlesconfiguring the powder is shown as a length of a long axis configuringthe particle, that is, a long axis length, (2) in a case where the shapeof the particle is a plate shape or a columnar shape (here, a thicknessor a height is smaller than a maximum long diameter of a plate surfaceor a bottom surface), the particle size is shown as a maximum longdiameter of the plate surface or the bottom surface, and (3) in a casewhere the shape of the particle is a sphere shape, a polyhedron shape,or an amorphous shape, and the long axis configuring the particlescannot be specified from the shape, the particle size is shown as anequivalent circle diameter. The equivalent circle diameter is a valueobtained by a circle projection method.

In addition, regarding an average acicular ratio of the powder, a lengthof a short axis, that is, a short axis length of the particles ismeasured in the measurement described above, a value of (long axislength/short axis length) of each particle is obtained, and anarithmetic average of the values obtained regarding 500 particles iscalculated. Here, unless otherwise noted, in a case of (1), the shortaxis length as the definition of the particle size is a length of ashort axis configuring the particle, in a case of (2), the short axislength is a thickness or a height, and in a case of (3), the long axisand the short axis are not distinguished, thus, the value of (long axislength/short axis length) is assumed as 1, for convenience.

In addition, unless otherwise noted, in a case where the shape of theparticle is specified, for example, in a case of definition of theparticle size (1), the average particle size is an average long axislength, and in a case of the definition (2), the average particle sizeis an average plate diameter. In a case of the definition (3), theaverage particle size is an average diameter (also referred to as anaverage particle diameter).

A content (filling percentage) of the ferromagnetic powder of themagnetic layer is preferably in a range of 50 to 90 mass % and morepreferably in a range of 60 to 90 mass %. A high filling percentage ofthe ferromagnetic powder in the magnetic layer is preferable from theviewpoint of improving recording density.

Binding Agent

The above-described magnetic recording medium may be a coating typemagnetic recording medium, and may include a binding agent in themagnetic layer. The binding agent is one or more resins. As the bindingagent, various resins usually used as a binding agent pf a coating typemagnetic recording medium can be used. For example, as the bindingagent, a resin selected from a polyurethane resin, a polyester resin, apolyamide resin, a vinyl chloride resin, an acrylic resin obtained bycopolymerizing styrene, acrylonitrile, or methyl methacrylate, acellulose resin such as nitrocellulose, an epoxy resin, a phenoxy resin,and a polyvinylalkylal resin such as polyvinyl acetal or polyvinylbutyral can be used alone or a plurality of resins can be mixed witheach other to be used. Among these, a polyurethane resin, an acrylicresin, a cellulose resin, and a vinyl chloride resin are preferable.These resins may be homopolymers or copolymers. These resins can be usedas the binding agent even in a non-magnetic layer and/or a back coatinglayer which will be described below.

For the binding agent described above, descriptions disclosed inparagraphs 0028 to 0031 of JP2010-024113A can be referred to. Regardingan average molecular weight of the resin used as the binding agent, thebinding agent can be used in an amount of, for example, 1.0 to 30.0parts by mass with respect to 100.0 parts by mass of the ferromagneticpowder.

Curing Agent

A curing agent can also be used together with the resin which can beused as the binding agent. As the curing agent, in an aspect, athermosetting compound which is a compound in which curing reaction(crosslinking reaction) proceeds due to heating can be used, and inanother aspect, a photocurable compound in which a curing reaction(crosslinking reaction) proceeds due to light irradiation can be used.Curing reaction proceeds during a process of forming a magnetic layer,whereby at least a part of the curing agent can be included in themagnetic layer in a state of being reacted (crosslinked) with othercomponents such as the binding agent. The same applies to the layerformed using this composition in a case where the composition used toform the other layer includes a curing agent. The preferred curing agentis a thermosetting compound, and polyisocyanate is suitable for this.For details of the polyisocyanate, descriptions disclosed in paragraphs0124 and 0125 of JP2011-216149A can be referred to. The curing agent canbe used in a magnetic layer forming composition in an amount of, forexample, 0 to 80.0 parts by mass, and preferably 50.0 to 80.0 parts bymass, from the viewpoint of improving a strength of the magnetic layer,with respect to 100.0 parts by mass of the binding agent.

Additive

The magnetic layer may include one or more kinds of additives, asnecessary. As the additives, the curing agent described above is used asan example. In addition, examples of the additive which can be includedin the magnetic layer include non-magnetic powder, a lubricant, adispersing agent, a dispersing assistant, a fungicide, an antistaticagent, and an antioxidant. For example, for the lubricant, descriptionsdisclosed in paragraphs 0030 to 0033, 0035, and 0036 of JP2016-126817Acan be referred to. The non-magnetic layer described later may include alubricant. For the lubricant which may be included in the non-magneticlayer, descriptions disclosed in paragraphs 0030, 0031, and 0034 to 0036of JP2016-126817A can be referred to. For the dispersing agent,descriptions disclosed in paragraphs 0061 and 0071 of JP2012-133837A canbe referred to.

Examples of the dispersing agent that can be added to the magnetic layerforming composition include a well-known dispersing agent for improvingthe dispersibility of ferromagnetic powder such as a carboxygroup-containing compound and a nitrogen-containing compound. Forexample, the nitrogen-containing compound may be any of a primary aminerepresented by NH₂R, a secondary amine represented by NHR₂, and atertiary amine represented by NR. In the above, R represents anystructure configuring the nitrogen-containing compound, and a pluralityof R's may be the same as or different from each other. Thenitrogen-containing compound may be a compound (polymer) having aplurality of repeating structures in the molecule. It is considered thata nitrogen-containing portion of the nitrogen-containing compoundfunctions as an adsorbing portion on the particle surface of theferromagnetic powder, which is the reason why the nitrogen-containingcompound can function as a dispersing agent. Examples of the carboxygroup-containing compound include a fatty acid such as oleic acid. It isconsidered that a carboxy group of the carboxy group-containing compoundfunctions as an adsorbing portion on the particle surface of theferromagnetic powder, which is the reason why the carboxygroup-containing compound can function as a dispersing agent. It is alsopreferable to use the carboxy group-containing compound and thenitrogen-containing compound in combination. The amount of thesedispersing agents used can be set appropriately.

The dispersing agent may be added to a non-magnetic layer formingcomposition. For the dispersing agent which can be included in thenon-magnetic layer forming composition, a description disclosed inparagraph 0061 of JP2012-133837A can be referred to.

Abrasive

As described above, it is considered that the number distribution A canbe an index of the existence state of the abrasive on the magnetic layersurface. Therefore, the number distribution A can be controlled by thekind of the non-magnetic powder added as the abrasive. As the abrasive,non-magnetic powder having a Mohs hardness of more than 8 is preferable,and non-magnetic powder having a Mohs hardness of 9 or more is morepreferable. A maximum value of a Mohs hardness is 10. The abrasive canbe powder of an inorganic substance and can also be powder of an organicsubstance. The abrasive can be inorganic or organic oxide powder orcarbide powder. Examples of the carbide include boron carbide (forexample, B₄C) and titanium carbide (for example, TiC). Diamond can alsobe used as the abrasive. In an aspect, the abrasive is preferablyinorganic oxide powder. Specifically, examples of the inorganic oxideinclude alumina (for example, Al₂O₃), titanium oxide (for example,TiO₂), cerium oxide (for example, CeO₂), and zirconium oxide (forexample, ZrO₂), among these, alumina is preferable. A Mohs hardness ofalumina is about 9. For the alumina powder, a description disclosed in aparagraph 0021 of JP2013-229090A can be referred to. A specific surfacearea can be used as an index of the particle size of the abrasive. Itcan be considered that the larger the specific surface area, the smallerthe particle size of the primary particles of particles configuring theabrasive. As the abrasive, it is preferable to use an abrasive having aspecific surface area (hereinafter, referred to as a “BET specificsurface area”.) measured by a Brunauer-Emmett-Teller (BET) method of 14m²/g or more. Further, from the viewpoint of the dispersibility, it ispreferable to use an abrasive having a BET specific surface area of 40m²/g or less. A content of the abrasive in the magnetic layer ispreferably 1.0 to 20.0 parts by mass, and more preferably 1.0 to 15.0parts by mass, with respect to 100.0 parts by mass of the ferromagneticpowder. As the abrasive, only one kind of non-magnetic powder can beused, and two or more kinds of non-magnetic powder having differentcompositions and/or physical properties (for example, size) can also beused. In a case where two or more kinds of non-magnetic powder are usedas the abrasive, the content of the abrasive means the total content ofthe two or more kinds of non-magnetic powder. The same applies tocontents of various components in the present invention and the presentspecification. The abrasive is preferably subjected to a dispersiontreatment separately from the ferromagnetic powder (separatedispersion), and more preferably subjected to a dispersion treatmentseparately from the filler described below (separate dispersion). In acase where the magnetic layer forming composition is prepared, it ispreferable to prepare two or more kinds of dispersion liquids havingdifferent components and/or dispersion conditions as a dispersion liquidof the abrasive (hereinafter, referred to as an “abrasive liquid”.) inorder to control the number distribution A.

A dispersing agent can also be used for adjusting the dispersion stateof the dispersion liquid of the abrasive. Examples of a compound thatcan function as a dispersing agent for improving the dispersibility ofthe abrasive include an aromatic hydrocarbon compound having a phenolichydroxy group. The “phenolic hydroxy group” refers to a hydroxy groupdirectly bonded to an aromatic ring. The aromatic ring included in thearomatic hydrocarbon compound may be a monocyclic ring, a polycyclicstructure, or a fused ring. From the viewpoint of improving thedispersibility of the abrasive, an aromatic hydrocarbon compoundincluding a benzene ring or a naphthalene ring is preferable. Further,the aromatic hydrocarbon compound may have a substituent other than thephenolic hydroxy group. Examples of the substituent other than thephenolic hydroxy group include a halogen atom, an alkyl group, an alkoxygroup, an amino group, an acyl group, a nitro group, a nitroso group,and a hydroxyalkyl group, and a halogen atom, an alkyl group, an alkoxygroup, an amino group, and a hydroxyalkyl group are preferable. Thenumber of phenolic hydroxy groups included in one molecule of thearomatic hydrocarbon compound may be one, two, three, or more.

A preferable aspect of the aromatic hydrocarbon compound having thephenolic hydroxy group includes a compound represented by Formula 100.

[In Formula 100, two of X¹⁰¹ to X¹⁰⁸ are hydroxy groups, and the othersix independently represent a hydrogen atom or a substituent.]

In the compound represented by Formula 100, the substitution positionsof two hydroxy groups (phenolic hydroxy groups) are not particularlylimited.

In the compound represented by Formula 100, two of X¹⁰¹ to X¹⁰⁸ arehydroxy groups (phenolic hydroxy groups), and the other sixindependently represent a hydrogen atom or a substituent. Further, inX¹⁰¹ to X¹⁰⁸, moieties other than the two hydroxy groups may all behydrogen atoms, or some or all of them may be substituents. As asubstituent, the substituent described above can be exemplified. As asubstituent other than the two hydroxy groups, one or more phenolichydroxy groups may be included. From the viewpoint of improving thedispersibility of the abrasive, it is preferable that the phenolichydroxy group is not used except for the two hydroxy groups of X¹⁰¹ toX¹⁰⁸. That is, the compound represented by Formula 100 is preferablydihydroxynaphthalene or a derivative thereof, and more preferably2,3-dihydroxynaphthalene or a derivative thereof. Examples of preferredsubstituents represented by X¹⁰¹ to X¹⁰⁸ include a halogen atom (forexample, a chlorine atom or a bromine atom), an amino group, an alkylgroup having 1 to 6 carbon atoms (preferably 1 to 4), a methoxy groupand an ethoxy group, an acyl group, a nitro group and a nitroso group,and —CH₂OH group.

For the dispersing agent for improving the dispersibility of theabrasive, descriptions disclosed in paragraphs 0024 to 0028 ofJP2014-179149A can be referred to.

The dispersing agent for improving the dispersibility of the abrasivecan be used, for example, in a proportion of 0.5 to 20.0 parts by mass,and is preferably used in a proportion of 1.0 to 10.0 parts by mass to100.0 parts by mass of the abrasive, for example, in a case where theabrasive liquid is prepared (for each abrasive liquid in a case where aplurality of the abrasive liquids are prepared).

Filler

As described above, it is considered that the number distribution B canbe an index of the existence state of the non-magnetic powder (filler)included in the magnetic layer on the magnetic layer surface in order toform appropriate protrusions on the magnetic layer surface forcontrolling friction characteristics. Therefore, the number distributionB can be controlled by the kind of the non-magnetic powder added as thefiller. An aspect of the filler includes carbon black. A BET specificsurface area of carbon black is preferably 10 m²/g or more, and morepreferably 15 m²/g or more. The BET specific surface area of carbonblack is preferably 50 m²/g or less, and more preferably 40 m²/g orless, from the viewpoint of the ease of improving the dispersibility. Inaddition, another aspect of the filler includes colloidal particles. Thecolloidal particles are preferably inorganic colloidal particles, morepreferably inorganic oxide colloidal particles, and still morepreferably silica colloidal particles (colloidal silica), from theviewpoint of availability. In the present invention and the presentspecification, the “colloidal particles” refer to particles which aredispersed without precipitation to generate a colloidal dispersion, in acase where 1 g of the particles is added to 100 mL of at least oneorganic solvent of methyl ethyl ketone, cyclohexanone, toluene, or ethylacetate, or a mixed solvent including two or more kinds of the solventdescribed above at an optional mixing ratio. An average particle size ofthe colloidal particles can be, for example, 30 to 300 nm, andpreferably 40 to 200 nm. A content of the filler in the magnetic layeris preferably 0.5 to 4.0 parts by mass, and more preferably 0.5 to 3.5parts by mass, with respect to 100.0 parts by mass of the ferromagneticpowder. The filler is preferably subjected to a dispersion treatmentseparately from the ferromagnetic powder, and more preferably subjectedto a dispersion treatment separately from the abrasive. In a case wherethe magnetic layer forming composition is prepared, it is preferable toprepare two or more kinds of dispersion liquids having differentcomponents and/or dispersion conditions as a dispersion liquid of thefiller (hereinafter, referred to as a “filler liquid”.) in order tocontrol the number distribution B.

From the viewpoint of improving the dispersibility of carbon black, inan aspect, a compound having an ammonium salt structure of an alkylester anion represented by Formula 1 can be used in a case where thefiller liquid is prepared. The “alkyl ester anion” can also be called an“alkyl carboxylate anion”.

In Formula 1, R represents an alkyl group having 7 or more carbon atomsor a fluorinated alkyl group having 7 or more carbon atoms, and Z⁺represents an ammonium cation.

From the viewpoint of improving the dispersibility of carbon black, inan aspect, two or more kinds of components capable of forming thecompound having a salt structure can be used in a case of preparing thefiller liquid. Thereby, in a case where the filler liquid is prepared,at least a part of these components can form the compound having a saltstructure.

Unless otherwise noted, groups described below may have a substituent ormay be unsubstituted. In addition, for a group having a substituent, theterm “carbon number” means the number of carbon atoms not including thenumber of carbon atoms of the substituent, unless otherwise noted. Inthe present invention and the present specification, examples of thesubstituent include an alkyl group (for example, an alkyl group having 1to 6 carbon atoms), a hydroxy group, an alkoxy group (for example, analkoxy group having 1 to 6 carbon atoms), a halogen atom (for example, afluorine atom, a chlorine atom, a bromine atom, or the like), a cyanogroup, an amino group, a nitro group, an acyl group, a carboxy group, asalt of a carboxy group, a sulfonic acid group, and a salt of a sulfonicacid group.

Hereinafter, Formula 1 will be described in more detail.

In Formula 1, R represents an alkyl group having 7 or more carbon atomsor a fluorinated alkyl group having 7 or more carbon atoms. Thefluorinated alkyl group has a structure in which some or all of thehydrogen atoms constituting the alkyl group are substituted withfluorine atoms. The alkyl group or the fluorinated alkyl grouprepresented by R may have a straight chain structure or a branchedstructure, may be a cyclic alkyl group or a fluorinated alkyl group, andis preferably a straight chain structure. The alkyl group or thefluorinated alkyl group represented by R may have a substituent, may beunsubstituted, and is preferably unsubstituted. The alkyl grouprepresented by R can be represented by, for example, C_(n)H_(2n+1)—.Here, n represents an integer of 7 or more. In addition, the fluorinatedalkyl group represented by R may have a structure in which some or allof the hydrogen atoms constituting the alkyl group represented by, forexample, C_(n)H_(2n+1)— are substituted with fluorine atoms. The carbonnumber of the alkyl group or the fluorinated alkyl group represented byR is 7 or more, preferably 8 or more, more preferably 9 or more, stillmore preferably 10 or more, still more preferably 11 or more, still morepreferably 12 or more, and still more preferably 13 or more. Inaddition, the carbon number of the alkyl group or the fluorinated alkylgroup represented by R is preferably 20 or less, more preferably 19 orless, and still more preferably 18 or less.

In Formula 1, Z⁺ represents an ammonium cation. Specifically, theammonium cation has the following structure. In the present inventionand the present specification, “*” in the formula representing a part ofa compound represents a bonding position between a structure of the partand an adjacent atom.

A nitrogen cation N⁺ of the ammonium cation and an oxygen anion O⁻ inFormula 1 may form a salt crosslinking group to form the ammonium saltstructure of the alkyl ester anion represented by Formula 1. Theinclusion of the compound having the ammonium salt structure of thealkyl ester anion represented by Formula 1 in the magnetic layer can beconfirmed by analyzing the magnetic recording medium by X-rayphotoelectron spectroscopy (electron spectroscopy for chemical analysis(ESCA)), infrared spectroscopy (IR), or the like.

In an aspect, the ammonium cation represented by Z⁺ may be provided, forexample, by a nitrogen atom of a nitrogen-containing polymer becoming acation. The nitrogen-containing polymer means a polymer including anitrogen atom. In the present invention and the present specification,the term “polymer” is used to encompass a homopolymer and a copolymer.The nitrogen atom may be included as an atom constituting a main chainof the polymer in an aspect, and may be included as an atom constitutinga side chain of the polymer in an aspect.

An aspect of the nitrogen-containing polymer includes polyalkyleneimine.Polyalkyleneimine is a ring-opening polymer of alkyleneimine and is apolymer having a plurality of repeating units represented by Formula 2.

A nitrogen atom N constituting a main chain in Formula 2 is a nitrogencation N⁺ to provide the ammonium cation represented by Z⁺ in Formula 1.Then, the ammonium salt structure can be formed with the alkyl esteranion, for example, as follows.

Hereinafter, Formula 2 will be described in more detail.

In Formula 2, R¹ and R² each independently represent a hydrogen atom oran alkyl group, and n1 represents an integer of 2 or more.

Examples of the alkyl group represented by R¹ or R² include an alkylgroup having 1 to 6 carbon atoms, preferably an alkyl group having 1 to3 carbon atoms, more preferably a methyl group or an ethyl group, andstill more preferably a methyl group. The alkyl group represented by R¹or R² is preferably an unsubstituted alkyl group. The combination of R¹and R² in Formula 2 may be a form in which one is a hydrogen atom andthe other is an alkyl group, a form in which both are hydrogen atoms,and a form in which both are alkyl groups (the same or different alkylgroups), and the form in which both are hydrogen atoms is preferable. Asthe alkyleneimine that provides the polyalkyleneimine, a structurehaving the lowest number of carbon atoms constituting a ring isethyleneimine, and the number of carbon atoms in a main chain of thealkyleneimine (ethyleneimine) obtained by the ring opening of theethyleneimine is 2. Therefore, n1 in Formula 2 is 2 or more. n1 inFormula 2 may be, for example, 10 or less, 8 or less, 6 or less, or 4 orless. The polyalkyleneimine may be a homopolymer including only the samestructure as the repeating structure represented by Formula 2, or may bea copolymer including two or more different structures as the repeatingstructure represented by Formula 2. A number-average molecular weight ofpolyalkyleneimine that can be used to form the compound having theammonium salt structure of the alkyl ester anion represented by Formula1 may be, for example, 200 or more, preferably 300 or more, and morepreferably 400 or more. The number-average molecular weight of thepolyalkyleneimine may be, for example, 10,000 or less, preferably 5,000or less, and more preferably 2,000 or less.

In the present invention and the present specification, the averagemolecular weight (weight-average molecular weight and number-averagemolecular weight) means a value measured by gel permeationchromatography (GPC) with standard polystyrene conversion. Unlessotherwise noted, the average molecular weight shown in Examplesdescribed below is a value (polystyrene-converted value) obtained bystandard polystyrene conversion of the values measured under thefollowing measurement conditions using GPC.

GPC device: HLC-8220 (manufactured by Tosoh Corporation)

Guard column: TSKguardcolumn Super HZM-H

Column: TSKgel Super HZ 2000, TSKgel Super HZ 4000, TSKgel Super HZ-M(manufactured by Tosoh Corporation, 4.6 mm (inner diameter)×15.0 cm,three columns connected in series)

Eluent: Tetrahydrofuran (THF), containing stabilizer(2,6-di-t-butyl-4-methylphenol)

Flow rate of eluent: 0.35 mL/min

Column temperature: 40° C.

Inlet temperature: 40° C.

Refractive index (RI) measurement temperature: 40° C.

Sample concentration: 0.3 mass %

Sample injection amount: 10 μL

Another aspect of the nitrogen-containing polymer includespolyallylamine. Polyallylamine is a polymer of allylamine and is apolymer having a plurality of repeating units represented by Formula 3.

A nitrogen atom N constituting an amino group of a side chain in Formula3 is a nitrogen cation N⁺ to provide the ammonium cation represented byZ⁺ in Formula 1. Then, the ammonium salt structure can be formed withthe alkyl ester anion, for example, as follows.

A weight-average molecular weight of polyallylamine that can be used toform the compound having the ammonium salt structure of the alkyl esteranion represented by Formula 1 may be, for example, 200 or more,preferably 1,000 or more, and more preferably 1,500 or more. Theweight-average molecular weight of the polyallylamine may be, forexample, 15,000 or less, preferably 10,000 or less, and more preferably8,000 or less.

The inclusion of a compound having a structure derived frompolyalkyleneimine or polyallylamine as the compound having the ammoniumsalt structure of the alkyl ester anion represented by Formula 1 in themagnetic layer can be confirmed by analyzing the magnetic layer surfaceby time-of-flight secondary ion mass spectrometry (TOF-SIMS) or thelike.

The compound having the ammonium salt structure of the alkyl ester anionrepresented by Formula 1 may be a salt of the nitrogen-containingpolymer and one or more kinds of fatty acids selected from the groupconsisting of fatty acids having 7 or more carbon atoms and fluorinatedfatty acids having 7 or more carbon atoms. The nitrogen-containingpolymer forming a salt may be one or more kinds of nitrogen-containingpolymers, and may be, for example, a nitrogen-containing polymerselected from the group consisting of polyalkyleneimine andpolyallylamine. The fatty acids forming a salt may be one or more kindsof fatty acids selected from the group consisting of fatty acids having7 or more carbon atoms and fluorinated fatty acids having 7 or morecarbon atoms. The fluorinated fatty acid has a structure in which someor all of the hydrogen atoms constituting an alkyl group bonded to acarboxy group COOH in the fatty acid are substituted with fluorineatoms. For example, the salt forming reaction can easily proceed bymixing the nitrogen-containing polymer and the above fatty acids at aroom temperature. A room temperature is, for example, about 20° C. to25° C. In an aspect, one or more kinds of nitrogen-containing polymersand one or more kinds of the above fatty acids are used as components ofthe filler liquid, and these are mixed in a process of preparing thefiller liquid to allow the salt forming reaction to proceed. Inaddition, in an aspect, the filler liquid can be prepared by mixing oneor more kinds of nitrogen-containing polymers and one or more kinds ofthe above fatty acids to form a salt before preparation of the fillerliquid, and then using the salt as a component of the filler liquid. Ina case where the nitrogen-containing polymer and the fatty acids aremixed to form an ammonium salt of the alkyl ester anion represented byFormula 1, in addition, a nitrogen atom constituting thenitrogen-containing polymer may react with a carboxy group of the fattyacids to form the following structure, and a form including such astructure is also included in the compound.

Examples of the fatty acids include fatty acids having an alkyl groupdescribed above as R in Formula 1 and fluorinated fatty acids having afluorinated alkyl group described above as R in Formula 1.

A mixing ratio of the nitrogen-containing polymer used to form thecompound having the ammonium salt structure of the alkyl ester anionrepresented by Formula 1 to the fatty acid is preferably 10:90 to 90:10,more preferably 20:80 to 85:15, and still more preferably 30:70 to 80:20as a mass ratio of the nitrogen-containing polymer:the fatty acids. Thecompound having the ammonium salt structure of the alkyl ester anionrepresented by Formula 1 can be used, for example, in an amount of 1.0to 20.0 parts by mass and is preferably used in an amount of 1.0 to 10.0parts by mass with respect to 100.0 parts by mass of the carbon black,in a case where the filler liquid is prepared (for each filler liquid ina case where a plurality of the filler liquids are prepared). Inaddition, in a case where the filler liquid is prepared (for each fillerliquid in a case where a plurality of the filler liquids are prepared),for example, 0.1 to 10.0 parts by mass of the nitrogen-containingpolymer can be used and 0.5 to 8.0 parts by mass of thenitrogen-containing polymer is preferably used, per 100.0 parts by massof the carbon black. The above fatty acids can be used, for example, inan amount of 0.05 to 10.0 parts by mass and are preferably used in anamount of 0.1 to 5.0 parts by mass, per 100.0 parts by mass of thecarbon black.

Non-Magnetic Layer

Next, the non-magnetic layer will be described. The above magneticrecording medium may have a magnetic layer directly on the surface ofthe non-magnetic support, or may have a magnetic layer on the surface ofthe non-magnetic support via a non-magnetic layer including non-magneticpowder. Non-magnetic powder used for the non-magnetic layer may beinorganic substance powder or organic substance powder. In addition,carbon black and the like can be used. Examples of the inorganicsubstance powder include types of powder of metal, metal oxide, metalcarbonate, metal sulfate, metal nitride, metal carbide, and metalsulfide. These types of non-magnetic powder can be purchased as acommercially available product or can be manufactured by a well-knownmethod. For details thereof, descriptions disclosed in paragraphs 0146to 0150 of JP2011-216149A can be referred to. For carbon black which canbe used in the non-magnetic layer, descriptions disclosed in paragraphs0040 and 0041 of JP2010-024113A can be referred to. A content (fillingpercentage) of the non-magnetic powder of the non-magnetic layer ispreferably in a range of 50 to 90 mass % and more preferably in a rangeof 60 to 90 mass %.

The non-magnetic layer can include a binding agent, and can also includean additive. For other details of a binding agent or an additive of thenon-magnetic layer, a well-known technology regarding the non-magneticlayer can be applied. In addition, in regards to the type and thecontent of the binding agent, and the type and the content of theadditive, for example, a well-known technology regarding the magneticlayer can be applied.

In the present invention and the present specification, the non-magneticlayer also includes a substantially non-magnetic layer including a smallamount of ferromagnetic powder as impurities, for example, orintentionally, together with the non-magnetic powder. Here, thesubstantially non-magnetic layer is a layer having a residual magneticflux density equal to or smaller than 10 mT, a layer having a coerciveforce equal to or smaller than 7.96 kA/m (100 Oe), or a layer having aresidual magnetic flux density equal to or smaller than 10 mT and acoercive force equal to or smaller than 7.96 kA/m (100 Oe). It ispreferable that the non-magnetic layer does not have a residual magneticflux density and a coercive force.

Non-Magnetic Support

Next, the non-magnetic support (hereinafter, referred to as a“support”.) will be described.

As the non-magnetic support, well-known components such as polyethyleneterephthalate, polyethylene naphthalate, polyamide, polyamide imide, andaromatic polyamide subjected to biaxial stretching are used. Amongthese, polyethylene terephthalate, polyethylene naphthalate, andpolyamide are preferable. These supports may be subjected to a coronadischarge, a plasma treatment, an easy-bonding treatment, or a thermaltreatment in advance.

Back Coating Layer

The magnetic recording medium may or may not have a back coating layerincluding non-magnetic powder on a surface side of the non-magneticsupport opposite to a surface side having the magnetic layer.Preferably, the back coating layer contains one or both of carbon blackand inorganic powder. The back coating layer can include a bindingagent, and can also include an additive. In regards to the binding agentand the additive of the back coating layer, the well-known technologyregarding the back coating layer can be applied, and the well-knowntechnology regarding the treatment of the magnetic layer and/or thenon-magnetic layer can be applied. For example, for the back coatinglayer, descriptions disclosed in paragraphs 0018 to 0020 ofJP2006-331625A and page 4, line 65 to page 5, line 38 of U.S. Pat. No.7,029,774B can be referred to.

Various Thicknesses

Regarding a thickness (total thickness) of the magnetic recordingmedium, it has been required to increase the recording capacity(increase the capacity) of the magnetic recording medium with theenormous increase in the amount of information in recent years. Forexample, as means for increasing the capacity of a tape-shaped magneticrecording medium (that is, a magnetic tape), a thickness of the magnetictape may be reduced to increase a length of the magnetic tapeaccommodated in one roll of a magnetic tape cartridge. From this point,the thickness (total thickness) of the magnetic recording medium ispreferably 5.6 μm or less, more preferably 5.5 μm or less, still morepreferably 5.4 μm or less, and still more preferably 5.3 μm or less. Inaddition, from the viewpoint of ease of handling, the thickness of themagnetic recording medium is preferably 3.0 μm or more, and morepreferably 3.5 μm or more.

The thickness (total thickness) of the magnetic recording medium can bemeasured by the following method.

Ten samples (for example, 5 to 10 cm in length) are cut out from anypart of the magnetic recording medium, and these samples are stacked tomeasure the thickness. A value (thickness per sample) obtained bydividing the measured thickness by 1/10 is set as the total thickness.The thickness measurement can be performed using a well-known measuringdevice capable of measuring the thickness on the order of 0.1 μm.

A thickness of the non-magnetic support is preferably 3.0 to 5.0 μm.

A thickness of the magnetic layer can be optimized according to asaturation magnetization amount, a head gap length, and a band of arecording signal of the used magnetic head, and is generally 0.01 μm to0.15 μm, and from the viewpoint of high density recording, is preferably0.02 μm to 0.12 μm, and more preferably 0.03 μm to 0.1 μm. The magneticlayer may be at least a single layer, the magnetic layer may beseparated into two or more layers having different magnetic properties,and a configuration of a well-known multilayered magnetic layer can beapplied as the magnetic layer. A thickness of the magnetic layer in acase where the magnetic layer is separated into two or more layers is atotal thickness of the layers.

A thickness of the non-magnetic layer is, for example, 0.1 to 1.5 μm,and preferably 0.1 to 1.0 μm.

A thickness of the back coating layer is preferably 0.9 μm or less, andmore preferably 0.1 to 0.7 μm.

Various thicknesses such as the thickness of the magnetic layer can beobtained by the following method.

A cross section of the magnetic recording medium in a thicknessdirection is exposed by an ion beam, and then the exposed cross sectionobservation is performed using a scanning electron microscope. Variousthicknesses can be obtained as an arithmetic average of thicknessesobtained at two optional points in the cross section observation.Alternatively, the thickness of each layer can be obtained as a designedthickness calculated according to manufacturing conditions.

Manufacturing Process

Preparation of Each Layer Forming Composition

A process of preparing a composition for forming a magnetic layer, anon-magnetic layer, or a back coating layer can usually include at leasta kneading process, a dispersing process, and a mixing process providedbefore and after these processes as necessary. Each process may bedivided into two or more stages. Components used for the preparation ofeach layer forming composition may be added at an initial stage or in amiddle stage of each process. As a solvent, one kind or two or morekinds of various solvents generally used for manufacturing a coatingtype magnetic recording medium can be used. For the solvent, forexample, a description disclosed in a paragraph 0153 of JP2011-216149Acan be referred to. In addition, each component may be separately addedin two or more processes. For example, a binding agent may be addedseparately in a kneading process, a dispersing process, and a mixingprocess for adjusting a viscosity after dispersion. In order tomanufacture the magnetic recording medium, a conventionally well-knownmanufacturing technology can be used in various processes. In thekneading process, preferably, a kneader having a strong kneading forcesuch as an open kneader, a continuous kneader, a pressure kneader, or anextruder is used. For details of the kneading treatment, descriptionsdisclosed in JP1989-106338A (JP-H01-106338A) and JP1989-079274A(JP-H01-079274A) can be referred to. As a dispersing device, awell-known dispersing device can be used. In any stage of preparing eachlayer forming composition, filtering may be performed by a well-knownmethod. The filtering can be performed by using a filter, for example.As the filter used for the filtering, a filter having a pore diameter of0.01 to 3 μm (for example, filter made of glass fiber or filter made ofpolypropylene) can be used, for example.

It is preferable that the abrasive liquid is prepared by beingseparately dispersed from the ferromagnetic powder and the filler. Thedispersion state of the abrasive in the abrasive liquid can be adjustedaccording to the use or non-use of a dispersing agent for improving thedispersibility of the abrasive, the amount of the dispersing agent used,treatment conditions of a dispersion treatment such as bead dispersion,and treatment conditions of a classification treatment such ascentrifugal separation. It is preferable to adjust the dispersion stateof the abrasive in order to control the number distribution A. Theabrasive liquid is preferably prepared as one or more kinds of abrasiveliquids including an abrasive, a solvent, and preferably a bindingagent, separately from the ferromagnetic powder and the filler, and canbe used for preparing a magnetic layer forming composition. Acommercially available device can be used for the dispersion treatmentand the classification treatment. Conditions for performing thesetreatments are not particularly limited, and need only be set accordingto the type of the device to be used so that the number distribution Asatisfies (1) to (3) described above.

In addition, it is preferable that the filler liquid is prepared bybeing separately dispersed from the ferromagnetic powder and theabrasive. The dispersion state of the filler in the filler liquid can beadjusted according to the use or non-use of a component for improvingthe dispersibility of the filler, the amount of the component used,treatment conditions of a dispersion treatment such as bead dispersion,and treatment conditions of a classification treatment such ascentrifugal separation. In an aspect, one or more kinds ofnitrogen-containing polymers and one or more kinds of the fatty acidsdescribed above are used as components of the filler liquid, and theseare mixed in a process of preparing the filler liquid to allow the saltforming reaction to proceed. In addition, in an aspect, the fillerliquid can be prepared by mixing one or more kinds ofnitrogen-containing polymers and one or more kinds of the above fattyacids to form a salt before preparation of the filler liquid, and thenusing the salt as a component of the filler liquid. It is preferable toadjust the dispersion state of the filler in order to control the numberdistribution B. The tiller liquid is preferably prepared as one or morekinds of abrasive liquids including a filler, a solvent, and preferablya binding agent, separately from the ferromagnetic powder and theabrasive, and can be used for preparing a magnetic layer formingcomposition. A commercially available device can be used for thestirring, the dispersion treatment, and the classification treatment.Conditions for performing these treatments are not particularly limited,and need only be set according to the type of the device to be used sothat the number distribution B satisfies (4) to (6) described above.

Regarding the dispersion treatment of the magnetic layer formingcomposition, in an aspect, the dispersion treatment of the ferromagneticpowder is performed by the two-stage dispersion treatment, in which thecoarse aggregation of the ferromagnetic powder is crushed by thefirst-stage dispersion treatment, and then the second-stage dispersiontreatment can be performed in which the collision energy applied to theparticles of the ferromagnetic powder by the collision with thedispersion beads is smaller than that in the first dispersion treatment.It is considered that such a dispersion treatment makes it possible toimprove the dispersibility of the ferromagnetic powder and suppress theoccurrence of chipping (partially lacking particles). This point ispreferable for controlling a vertical squareness ratio, as describedbelow.

An example of the two-stage dispersion treatment includes a dispersiontreatment including a first stage of obtaining a dispersion liquid bysubjecting ferromagnetic powder, a binding agent, and a solvent to adispersion treatment in the presence of first dispersion beads and asecond stage of subjecting the dispersion liquid obtained in the firststage to a dispersion treatment in the presence of second dispersionbeads having a smaller bead diameter and density than the firstdispersion beads. Hereinafter, the above dispersion treatment will befurther described.

In order to improve the dispersibility of the ferromagnetic powder, itis preferable that the first stage and the second stage described aboveare performed as a dispersion treatment before mixing the ferromagneticpowder with other powder components. For example, the first stage andthe second stage are preferably performed as a dispersion treatment of aliquid (magnetic liquid) including ferromagnetic powder, a bindingagent, a solvent, and an optionally added additive before mixing theferromagnetic powder with the abrasive and the filler.

The bead diameter of the second dispersion beads is preferably 1/100 orless of the bead diameter of the first dispersion beads, and morepreferably 1/500 or less of the bead diameter of the first dispersionbeads. In addition, the bead diameter of the second dispersion beads maybe, for example, 1/10,000 or more of the bead diameter of the firstdispersion beads. However, it is not limited to this range. For example,the bead diameter of the second dispersion beads is preferably in arange of 80 to 1,000 nm. On the other hand, the bead diameter of thefirst dispersion beads may be, for example, in a range of 0.2 to 1.0 mm.

In the present invention and the present specification, the beaddiameter is a value measured by the same method as a method formeasuring an average particle size of powder described above.

The second stage is preferably performed under a condition that, on amass basis, the second dispersion beads are present in an amount of 10times or more the amount of ferromagnetic hexagonal ferrite powder, andmore preferably performed under a condition that the second dispersionbeads are present in an amount of 10 times to 30 times the amount offerromagnetic hexagonal ferrite powder.

On the other hand, the amount of the first dispersion beads in the firststage is also preferably in the above range.

The second dispersion beads are beads having a density lower than thatof the first dispersion beads. The “density” is obtained by dividing themass (unit: g) of the dispersion beads by the volume (unit: cm³). Themeasurement is performed by an Archimedes method. The density of thesecond dispersion beads is preferably 3.7 g/cm³ or less, and morepreferably 3.5 g/cm³ or less. The density of the second dispersion beadsmay be, for example, 2.0 g/cm³ or more, and may be lower than 2.0 g/cm³.Preferred second dispersion beads in terms of the density includediamond beads, silicon carbide beads, silicon nitride beads and thelike, and preferred second dispersion beads in terms of the density andthe hardness include diamond beads.

On the other hand, as the first dispersion beads, dispersion beadshaving a density of more than 3.7 g/cm³ are preferable, dispersion beadshaving a density of 3.8 g/cm³ or more are more preferable, anddispersion beads having a density of 4.0 g/cm³ or more are still morepreferable. The density of the first dispersion beads may be, forexample, 7.0 g/cm³ or less, and may be more than 7.0 g/cm³. As the firstdispersion beads, zirconia beads, alumina beads, and the like arepreferably used, and zirconia beads are more preferably used.

The dispersion time is not particularly limited and need only be setaccording to the type of the dispersing device used.

Coating Process

The magnetic layer can be formed by directly applying the magnetic layerforming composition onto the surface of the non-magnetic support orperforming multilayer applying of the magnetic layer forming compositionwith the non-magnetic layer forming composition in order or at the sametime. The back coating layer can be formed by applying the back coatinglayer forming composition onto a surface of the non-magnetic supportopposite to a surface having the non-magnetic layer and/or the magneticlayer (or to be provided with the non-magnetic layer and/or the magneticlayer). For details of coating for forming each layer, a descriptiondisclosed in a paragraph 0066 of JP2010-231843A can be referred to.

Other Processes

Well-known technologies can be applied to other various processes formanufacturing the magnetic recording medium. For the various processes,for example, descriptions disclosed in paragraphs 0067 to 0070 ofJP2010-231843A can be referred to. For example, a coating layer of themagnetic layer forming composition can be subjected to an orientationtreatment in an orientation zone while the coating layer is in a wetstate. For the orientation treatment, the various well-knowntechnologies including a description disclosed in a paragraph 0052 ofJP2010-024113A can be used. For example, a vertical orientationtreatment can be performed by a well-known method such as a method usinga polar opposing magnet. In the orientation zone, a drying speed of thecoating layer can be controlled depending on a temperature and a flowrate of dry air and/or a transportation speed in the orientation zone.The coating layer may be preliminarily dried before the transportationto the orientation zone. As an example, a magnetic field intensity inthe vertical orientation treatment may be 0.1 to 1.5 T. The higher themagnetic field intensity in the vertical orientation treatment, thelarger the vertical squareness ratio value and the vertical coerciveforce value, which will be described below in detail.

The magnetic recording medium according to an aspect of the presentinvention may be a tape-shaped magnetic recording medium (magnetic tape)or a disk-shaped magnetic recording medium (magnetic disk). For example,for the magnetic tape, a long magnetic tape original roll can beobtained through various processes. The obtained magnetic tape originalroll is cut (slit) by a well-known cutter to have a width of themagnetic tape to be wound around the magnetic tape cartridge. The widthis determined according to the standard, and is typically ½ inches. ½inches=12.65 mm. A servo pattern is usually formed on the magnetic tapeobtained by slitting. Details of the servo pattern will be describedbelow. The magnetic tape is usually accommodated in a magnetic tapecartridge and the magnetic tape cartridge is mounted in the magneticrecording and reproducing apparatus.

Formation of Servo Pattern

It is possible to form a servo pattern in the magnetic recording mediumby a well-known method in order to enable tracking control of themagnetic head in the magnetic recording and reproducing apparatus,control of a running speed of the magnetic recording medium, and thelike. The “formation of the servo pattern” can also be referred to as“recording of a servo signal”. Hereinafter, the formation of the servopatterns will be described using a magnetic tape as an example.

The servo pattern is usually formed along a longitudinal direction ofthe magnetic tape. Examples of control (servo control) types using aservo signal include a timing-based servo (TBS), an amplitude servo, anda frequency servo.

As shown in a european computer manufacturers association (ECMA)-319(June 2001), a magnetic tape conforming to a linear tape-open (LTO)standard (generally referred to as an “LTO tape”.) employs atiming-based servo system. In the timing-based servo system, the servopattern is formed by continuously disposing a plurality of pairs ofnon-parallel magnetic stripes (also referred to as “servo stripes”.) ina longitudinal direction of the magnetic tape. As described above, thereason why the servo pattern is formed of a pair of non-parallelmagnetic stripes is to indicate, to a servo signal reading elementpassing over the servo pattern, a passing position thereof.Specifically, the pair of magnetic stripes is formed so that an intervalthereof continuously changes along a width direction of the magnetictape, and the servo signal reading element reads the interval to therebysense a relative position between the servo pattern and the servo signalreading element. Information on this relative position enables trackingon a data track. Therefore, a plurality of servo tracks are usually seton the servo pattern along a width direction of the magnetic tape.

A servo band is formed of servo signals continuous in a longitudinaldirection of the magnetic tape. A plurality of the servo bands areusually provided on the magnetic tape. For example, in an LTO tape, thenumber is five. A region interposed between two adjacent servo bands isreferred to as a data band. The data band is formed of a plurality ofdata tracks, and each data track corresponds to each servo track.

Further, in an aspect, as shown in JP2004-318983A, informationindicating a servo band number (referred to as “servo bandidentification (ID)” or “unique data band identification method (UDIM)information”.) is embedded in each servo band. This servo band ID isrecorded by shifting a specific one of the plurality of pairs of theservo stripes in the servo band so that positions thereof are relativelydisplaced in a longitudinal direction of the magnetic tape.Specifically, a way of shifting the specific one of the plurality ofpairs of servo stripes is changed for each servo band. Accordingly, therecorded servo band ID is unique for each servo band, and thus, theservo band can be uniquely specified only by reading one servo band witha servo signal reading element.

Incidentally, as a method for uniquely specifying the servo band, thereis a method using a staggered method as shown in ECMA-319 (June 2001).In this staggered method, a group of pairs of non-parallel magneticstripes (servo stripes) disposed continuously in plural in alongitudinal direction of the magnetic tape is recorded so as to beshifted in a longitudinal direction of the magnetic tape for each servoband. Since this combination of shifting methods between adjacent servobands is unique throughout the magnetic tape, it is possible to uniquelyspecify a servo band in a case of reading a servo pattern with two servosignal reading elements.

As shown in ECMA-319 (June 2001), information indicating a position ofthe magnetic tape in the longitudinal direction (also referred to as“longitudinal position (LPOS) information”) is usually embedded in eachservo band. This LPOS information is also recorded by shifting thepositions of the pair of servo stripes in the longitudinal direction ofthe magnetic tape, as the UDIM information. Here, unlike the UDIMinformation, in this LPOS information, the same signal is recorded ineach servo band.

It is also possible to embed, in the servo band, the other informationdifferent from the above UDIM information and LPOS information. In thiscase, the embedded information may be different for each servo band asthe UDIM information or may be common to all servo bands as the LPOSinformation.

As a method of embedding information in the servo band, it is possibleto employ a method other than the above. For example, a predeterminedcode may be recorded by thinning out a predetermined pair from the groupof pairs of servo stripes.

A servo pattern forming head is called a servo write head. The servowrite head has a pair of gaps corresponding to the pair of magneticstripes as many as the number of servo bands. Usually, a core and a coilare connected to each pair of gaps, and by supplying a current pulse tothe coil, a magnetic field generated in the core can cause generation ofa leakage magnetic field in the pair of gaps. In a case of forming theservo pattern, by inputting a current pulse while running the magnetictape on the servo write head, the magnetic pattern corresponding to thepair of gaps is transferred to the magnetic tape to form the servopattern. A width of each gap can be appropriately set according to adensity of the servo pattern to be formed. The width of each gap can beset to, for example, 1 μm or less, 1 to 10 μm, 10 μm or more, and thelike.

Before the servo pattern is formed on the magnetic tape, the magnetictape is usually subjected to demagnetization (erasing) treatment. Thiserasing treatment can be performed by applying a uniform magnetic fieldto the magnetic tape using a direct current magnet or an alternatingcurrent magnet. The erasing treatment includes direct current (DC)erasing and alternating current (AC) erasing. The AC erasing isperformed by gradually decreasing an intensity of the magnetic fieldwhile inverting a direction of the magnetic field applied to themagnetic tape. On the other hand, the DC erasing is performed byapplying a one-direction magnetic field to the magnetic tape. As the DCerasing, there are two methods. A first method is horizontal DC erasingof applying a one-direction magnetic field along a longitudinaldirection of the magnetic tape. A second method is vertical DC erasingof applying a one-direction magnetic field along a thickness directionof the magnetic tape. The erasing treatment may be performed on theentire magnetic tape or may be performed for each servo band of themagnetic tape.

A direction of the magnetic field of the servo pattern to be formed isdetermined according to a direction of the erasing. For example, in acase where the horizontal DC erasing is performed on the magnetic tape,the servo pattern is formed so that the direction of the magnetic fieldis reverse to the direction of the erasing. Therefore, an output of aservo signal obtained by reading the servo pattern can be increased. Asshown in JP2012-053940A, in a case where a magnetic pattern istransferred to, using the gap, a magnetic tape that has been subjectedto vertical DC erasing, a servo signal obtained by reading the formedservo pattern has a monopolar pulse shape. On the other hand, in a casewhere a magnetic pattern is transferred to, using the gap, a magnetictape that has been subjected to horizontal DC erasing, a servo signalobtained by reading the formed servo pattern has a bipolar pulse shape.

Vertical Squareness Ratio

In an aspect, a vertical squareness ratio of the magnetic recordingmedium may be 0.65 or more and 1.00 or less. In the present inventionand the present specification, the “vertical squareness ratio” is asquareness ratio measured in the vertical direction of the magneticrecording medium. The “vertical direction” described regarding thesquareness ratio and the coercive force described below is a directionorthogonal to the magnetic layer surface, and can also be referred to asa thickness direction. The vertical squareness ratio is measured using avibrating sample magnetometer. More specifically, the verticalsquareness ratio in the present invention and the present specificationis a value obtained by sweeping an external magnetic field on themagnetic recording medium under conditions of a maximum externalmagnetic field of 15 kOe and a scanning speed of 60 Oe/sec at ameasurement temperature of 23° C.±1° C. using a vibrating samplemagnetometer, the value being after diamagnetic field correction. Themeasured value is obtained as a value obtained by subtracting themagnetization of a sample probe of the vibrating sample magnetometer asa background noise.

It is preferable that the number distribution A and the numberdistribution B of the magnetic recording medium are the above-describeddistributions from the viewpoint of improving the electromagneticconversion characteristics in reproducing data recorded on the magneticrecording medium, in addition to a favorable reproduction quality in theGTT described above. This is because it is considered that the presenceof non-magnetic powder, which is a non-magnetic component, so as tosatisfy such a distribution can contribute to the narrowing of the widthof a magnetization transition region during recording of data on themagnetic recording medium. The fact that the width of the magnetizationtransition region can be narrowed is effective in improving theelectromagnetic conversion characteristics. Further, since the steepmagnetic distribution of the magnetic recording medium can contribute tothe narrowing of the width of the magnetization transition region, it ispreferable from this point that the vertical squareness ratio of themagnetic recording medium is 0.65 or more and 1.00 or less. From thispoint, the vertical squareness ratio of the magnetic recording medium ispreferably 0.65 or more, more preferably 0.70 or more, and still morepreferably 0.80 or more. The squareness ratio is 1.00 at maximum inprinciple. Therefore, the vertical squareness ratio of the magneticrecording medium is 1.00 or less. The vertical squareness ratio of themagnetic recording medium may be, for example, 0.95 or less, 0.90 orless, 0.87 or less, or 0.85 or less. The larger the vertical squarenessratio value of the magnetic recording medium, the more preferable fromthe viewpoint of improving the electromagnetic conversioncharacteristics. The vertical squareness ratio of the magnetic recordingmedium may be more than the value exemplified above. Further, from theviewpoint of improving the electromagnetic conversion characteristics,it is more preferable to record data by combining a recording element tobe described in detail later and the magnetic recording medium.

Vertical Coercive Force

In an aspect, a vertical coercive force of the magnetic recording mediummay be 2,500 Oe or more and 3,500 Oe or less. In the present inventionand the present specification, the “vertical coercive force” is acoercive force measured in the vertical direction of the magneticrecording medium. In the present invention and the presentspecification, the vertical coercive force is a value obtained bysweeping an external magnetic field on the magnetic recording mediumunder conditions of a maximum external magnetic field of 15 kOe and ascanning speed of 60 Oe/sec at a measurement temperature of 23° C. 1° C.using a vibrating sample magnetometer. The measured value is obtained asa value obtained by subtracting the magnetization of a sample probe ofthe vibrating sample magnetometer as a background noise. In terms ofunits, 1 Oe (1 oersted)=79.6 A/m.

As described above, it is preferable that the number distribution A andthe number distribution B of the magnetic recording medium are theabove-described distributions from the viewpoint of improving theelectromagnetic conversion characteristics in reproducing data recordedon the magnetic recording medium, in addition to a favorablereproduction quality in the GTT described above. Further, from theviewpoint of improving the electromagnetic conversion characteristics,it is preferable that the vertical coercive force of the magneticrecording medium is 3,500 Oe or less in combination with a recordingelement having a write gap length of 120 nm or less. This is for thefollowing reason. Since a recording element having a small write gaplength can increase a recording magnetic field gradient applicable tothe magnetic recording medium, it can contribute to the narrowing of thewidth of the magnetization transition region. From this point, therecording element having a write gap length of 120 nm or less ispreferable. On the other hand, although the recording magnetic fieldgradient can be increased by using such a recording element, a recordingmagnetic field intensity tends to decrease. In such a case, the verticalcoercive force of the magnetic recording medium of 3,500 Oe or less maycontribute to the improvement of the electromagnetic conversioncharacteristics. From this point, the vertical coercive force is morepreferably 3,200 Oe or less, and still more preferably 3,000 Oe or less.On the other hand, in order to improve the electromagnetic conversioncharacteristics, it is preferable that the magnetic stability is high,and from this point, the vertical coercive force of the magneticrecording medium is preferably 2,500 Oe or more, and more preferably2,700 Oe or more.

Magnetic Tape Cartridge

An aspect of the present invention relates to a magnetic tape cartridgeincluding the magnetic recording medium that is a magnetic tape.

The details of the magnetic tape included in the above tape cartridgeare as described above.

In the magnetic tape cartridge, generally, the magnetic tape isaccommodated inside a cartridge body in a state of being wound around areel. The reel is rotatably provided inside the cartridge body. As themagnetic tape cartridge, a single reel type magnetic tape cartridgehaving one reel inside the cartridge body and a dual reel type magnetictape cartridge having two reels inside the cartridge body are widelyused. In a case where the single reel type magnetic tape cartridge ismounted on a magnetic tape apparatus for recording and/or reproducingdata on the magnetic tape, the magnetic tape is pulled out of themagnetic tape cartridge to be wound around the reel on the magnetic tapeapparatus side. A magnetic head is disposed on a magnetic tapetransportation path from the magnetic tape cartridge to a winding reel.Feeding and winding of the magnetic tape are performed between a reel(supply reel) on the magnetic tape cartridge side and a reel (windingreel) on the magnetic tape apparatus side. During this time, data isrecorded and/or reproduced as the magnetic head and the magnetic layersurface of the magnetic tape come into contact with each other to beslid on each other. With respect to this, in the dual reel type magnetictape cartridge, both reels of the supply reel and the winding reel areprovided in the magnetic tape cartridge.

Magnetic Tape Cartridge Group

An aspect of the present invention relates to a magnetic tape cartridgegroup including a plurality of the magnetic tape cartridges.

The magnetic tape cartridge group includes a plurality of the magnetictape cartridges including magnetic tapes in which the numberdistribution A satisfies the above (1) to (3) and the numberdistribution B satisfies the above (4) to (6). The number of magnetictape cartridges included (referred to as the “number of rolls”) may be200 or more, 1,000 or more, or 3,000 or more. In an aspect, the numberof rolls may be, for example, 5,000 or less or 4,000 or less. Themagnetic tape cartridge group may be, for example, a magnetic tapecartridge group sold by the same manufacturer as a magnetic tapecartridge for the same standard.

In the magnetic tape cartridge group, in an environment of an atmospheretemperature of 21° C. and a relative humidity of 50%, a slope α (GTTslope α) of a signal-to-noise-ratio with respect to the number of rolls,the slope α being obtained by performing a reproduction test of a totalof 200 rolls of the magnetic tape cartridges using a single magnetichead, is preferably 0.5 dB/decade or less, more preferably 0.4 dB/decadeor less, and still more preferably 0.3 dB/decade or less, from theviewpoint of obtaining a favorable reproduction quality in the GTT underan environment of about room temperature. The GTT slope α may be, forexample, 0 dB/decade or more, more than 0 dB/decade, or 0.1 dB/decade ormore. A smaller value of the GTT slope α is preferable from theviewpoint of obtaining the more favorable reproduction quality in theGTT under an environment of about room temperature.

The GTT slope α is obtained by the following method.

In a case where the magnetic tape cartridge group to be measuredconsists of 200 rolls of the magnetic tape cartridges, all magnetic tapecartridges are used. In a case where the magnetic tape cartridge groupto be measured consists of the magnetic tape cartridges having thenumber of rolls more than 200, randomly extracted 200 rolls of themagnetic tape cartridges are used. Each magnetic tape cartridge used forevaluation is randomly assigned a number from 1 to 200.

In an environment of an atmosphere temperature of 21° C. and a relativehumidity of 50%, an average value of all channels of thesignal-to-noise-ratio (SNR) for each magnetic tape cartridge isevaluated by an LTO8 drive. The evaluation result is analyzed by a leastsquare method (logarithmic approximation). Specifically, the axis ofabscissa (X axis) of the graph represents the logarithmic of thecartridge number, the axis of ordinate (Y axis) represents the SNR(average value of all channels) obtained for each magnetic tapecartridge, and these points are linearly approximated by the leastsquare method. Thus, the GTT slope α (unit: dB/decade) is obtained as aslope α of Y=αX+β (α is a slope and β is an intercept).

Further, an aspect of the present invention relates to a magnetic tapecartridge group in which the GTT slope α obtained by the above method is0.5 dB/decade or less. The above description can be referred to for thedetails of the magnetic tape cartridge group.

Magnetic Recording and Reproducing Apparatus

An aspect of the present invention relates to a magnetic recording andreproducing apparatus including the magnetic recording medium.

In the present invention and the present specification, the “magneticrecording and reproducing apparatus” means an apparatus capable ofperforming at least one of the recording of data on the magneticrecording medium or the reproducing of data recorded on the magneticrecording medium. Such an apparatus is generally called a drive. Themagnetic recording and reproducing apparatus can be a sliding typemagnetic recording and reproducing apparatus. The sliding type magneticrecording and reproducing apparatus is an apparatus in which themagnetic layer surface and the magnetic head come into contact with eachother to be slid on each other, in a case of performing the recording ofdata on the magnetic recording medium and/or reproducing of the recordeddata. For example, the magnetic recording and reproducing apparatus canattachably and detachably include the magnetic tape cartridge.

The magnetic head included in the magnetic recording and reproducingapparatus can be a recording head capable of performing the recording ofdata on the magnetic recording medium, or can be a reproducing headcapable of performing the reproducing of data recorded on the magneticrecording medium. In addition, in an aspect, the magnetic recording andreproducing apparatus can include both of a recording head and areproducing head as separate magnetic heads. In another aspect, themagnetic head included in the magnetic recording and reproducingapparatus can have a configuration that both of an element for recordingdata (recording element) and an element for reproducing data(reproducing element) are included in one magnetic head. Hereinafter,the element for recording and the element for reproducing data arecollectively referred to as an “element for data”. As the reproducinghead, a magnetic head (MR head) including a magnetoresistive (MR)element capable of sensitively reading data recorded on the magnetictape as a reproducing element is preferable. As the MR head, variouswell-known MR heads such as an anisotropic magnetoresistive (AMR) head,a giant magnetoresistive (GMR) head, and a tunnel magnetoresistive (TMR)head can be used. In addition, the magnetic head which performs therecording of data and/or the reproducing of data may include a servosignal reading element. Alternatively, as a head other than the magnetichead which performs the recording of data and/or the reproducing ofdata, a magnetic head (servo head) comprising a servo signal readingelement may be included in the magnetic recording and reproducingapparatus. For example, a magnetic head that records data and/orreproduces recorded data (hereinafter also referred to as “recording andreproducing head”.) can include two servo signal reading elements, andthe two servo signal reading elements can read two adjacent servo bandssimultaneously. One or a plurality of elements for data can be disposedbetween the two servo signal reading elements.

In the magnetic recording and reproducing apparatus, recording of dataon the magnetic recording medium and/or reproducing of data recorded onthe magnetic recording medium can be performed as the magnetic layersurface of the magnetic recording medium and the magnetic head come intocontact with each other to be slid on each other. The above magneticrecording and reproducing apparatus need only include the magneticrecording medium according to one aspect of the present invention, andthe well-known technology can be applied to the others.

For example, in a case where data is recorded on the magnetic recordingmedium on which a servo pattern is formed and/or recorded data isreproduced, first, tracking is performed using a servo signal obtainedby reading the servo pattern. That is, by causing the servo signalreading element to follow a predetermined servo track, the element fordata is controlled to pass over the target data track. Displacement ofthe data track is performed by changing a servo track to be read by theservo signal reading element in a tape width direction.

The recording and reproducing head can also perform recording and/orreproducing with respect to other data bands. In this case, the servosignal reading element may be displaced to a predetermined servo bandusing the above described UDM information, and tracking for the servoband may be started.

In the magnetic recording and reproducing apparatus, for example, a OTTcan be performed while replacing the magnetic recording medium (forexample, a magnetic tape cartridge) with a new one. The magneticrecording medium according to an aspect of the present invention cancontribute to obtaining a favorable reproduction quality in a green tapetest (GT) under an environment of about room temperature.

In an aspect, the recording element can be an inductive recordingelement. The inductive recording element is generally called anelectromagnetic induction recording element or a magnetic inductionrecording element. In the inductive recording element, a current ispassed through a coil to generate a leakage magnetic field from a gapportion (write gap) of a head core, and a magnetization region is formed(that is, data is recorded) in a magnetic layer by the leakage magneticfield. Regarding the recording element, in an aspect, it is preferablethat the recording element is an inductive recording element having thefollowing configuration (hereinafter, referred to as a “recordingelement a”.) from the viewpoint of improving the electromagneticconversion characteristics in reproducing data recorded on the magneticrecording medium, in addition to a favorable reproduction quality in theOTT described above.

-   -   The inductive recording element has a first magnetic pole that        generates a magnetic field and a second magnetic pole that is        separated from the first magnetic pole with a write gap        therebetween,    -   in which the first magnetic pole has a layer made of an alloy        containing Co and Fe as an outermost layer of a portion facing        the second magnetic pole with the write gap therebetween, and    -   the second magnetic pole has a layer made of an alloy containing        Co and Fe as an outermost layer of a portion facing the first        magnetic pole with the write gap therebetween.

In addition, in an aspect, it is preferable that the recording elementis an inductive recording element having a write gap length of 120 nm orless (hereinafter, referred to as a “recording element b”.) from theviewpoint of improving the electromagnetic conversion characteristics inreproducing data recorded on the magnetic recording medium, in additionto a favorable reproduction quality in the GTT described above. Thewrite gap length is generally also called a recording gap length. Thewrite gap length may be 110 nm or less, or 100 nm or less. In addition,from the viewpoint of the recording magnetic field intensity, the writegap length is preferably 60 nm or more, and more preferably 70 nm ormore.

It is also preferable that the recording element a has the configurationof the recording element b.

The recording element a and the recording element b can have the sameconfiguration as a well-known inductive recording element, except thatthe recording element a and the recording element b have the aboveconfiguration. For the configuration of a well-known inductive recordingelement, for example, FIGS. 1 to 6 and the description of these drawingsof US2011/0273797A 1 can be referred to.

Hereinafter, the recording element a will be described in more detailwith reference to the drawings. Here, one embodiment shown in thedrawings is an example, and the recording element a is not limited tothe exemplified aspect.

FIG. 1 is a partially enlarged view of an example of the recordingelement. In FIG. 1, a further partially enlarged view of the leftdiagram is the right diagram. In the left diagram of FIG. 1, a dottedarrow indicates a running direction of the magnetic recording medium ina case where data is recorded on the magnetic recording medium. Arecording element 10 shown in FIG. 1 includes a first magnetic pole 11,a second magnetic pole 12, and a coil 13. The second magnetic pole 12 isseparated from the first magnetic pole 11 with a write gap Gtherebetween.

The first magnetic pole 11 is a magnetic pole generally called a leadingside magnetic pole, and is a magnetic pole that generates a magneticfield. The magnetic field generated from the first magnetic pole leaksfrom the write gap to form a leakage magnetic field, and data isrecorded on the magnetic recording medium by the leakage magnetic field.

By passing a current through the coil 13, the magnetic field can begenerated by passing a magnetic flux through the first magnetic pole 11.

The second magnetic pole 12 is a magnetic pole generally called atrailing side magnetic pole, and is a magnetic pole that closes amagnetic path with respect to the magnetic recording medium.

FIG. 2 is a schematic cross-sectional view showing a configuration of awrite gap-side tip portion of the recording element 10 shown in FIG. 1.The first magnetic pole 11 has an outermost layer 111 on a base material110. The second magnetic pole 12 has an outermost layer 121 on the basematerial 120. The outermost layer 111 and the outermost layer 121 arelayers made of an alloy containing Co and Fe, respectively. The presentinventor supposes that the fact that such layers are positioned on boththe magnetic poles as the outermost layers facing each other with thewrite gap therebetween can contribute to providing a high recordingmagnetic field and a high recording magnetic field gradient during datarecording. The present inventor considers that this is because the alloycontaining Co and Fe generally tends to have a higher saturationmagnetic flux density than the alloy constituting the magnetic pole ofthe recording element. From the viewpoint of obtaining a highersaturation magnetic flux density, in the composition of the above alloy,the Co content is preferably in a range of 10% to 60%, and the Fecontent is preferably in a range of 20% to 90% on an at % basis. Inaddition, the above alloy more preferably contains Ni, and in thecomposition of the above alloy, the Ni content is still more preferablyin a range of 5% to 50% on an at % basis. A thickness of the outermostlayer is preferably 10 nm or more, and more preferably 30 nm or more. Inaddition, the thickness of the outermost layer may be, for example, 300nm or less or 200 nm or less. The outermost layer can be formed by awell-known film forming method for forming an alloy film, such assputtering or vapor deposition. The outermost layer need only beprovided at a portion of each magnetic pole facing the other magneticpole with at least the write gap therebetween. The base material 110 ofthe first magnetic pole 11 and the base material 120 of the secondmagnetic pole 12 can each be an alloy base material that constitutes amagnetic pole of a normal recording element. Examples of such an alloyinclude an alloy containing Fe and Ni. Examples of such an alloy includean FeNi alloy generally called permalloy. The permalloy is an alloy ofFe and Ni containing 35% to 80% of Ni on an at % basis.

The number and arrangement of the recording elements included in themagnetic head can be determined according to the standard of themagnetic recording and reproducing apparatus.

The recording element a and the recording element b can contribute tothe improvement of the electromagnetic conversion characteristics inreproducing data recorded on the magnetic recording medium, and can alsocontribute to the improvement of the electromagnetic conversioncharacteristics in recording and reproducing data at a high recordingdensity. The recording density may be, for example, 200 kfci or more(for example, in a range of 200 to 600 kfci) as a linear recordingdensity. The unit kfci is a unit of the linear recording density (cannotbe converted into an SI unit system).

EXAMPLES

Hereinafter, the present invention will be described based on Examples.Here, the present invention is not limited to aspects shown in Examples.Unless otherwise specified, “parts” and “%” in the following descriptionindicate “parts by mass” and “mass %”. The processes and evaluations inthe following description were performed in an environment of anatmosphere temperature of 23° C. 1° C., unless otherwise noted. Inaddition, “eq” described below indicates an equivalent that is a unitthat cannot be converted into an SI unit system.

Preparation of Abrasive Liquid

Preparation of Abrasive Liquid A

2,3-dihydroxynaphthalene (manufactured by Tokyo Chemical Industry Co.,Ltd.) having the amount shown in Table 1, 31.3 parts of a 32% solution(solvent is a mixed solvent of methyl ethyl ketone and toluene) of apolyester polyurethane resin having a SO₃Na group as a polar group(UR-4800 manufactured by Toyobo Co., Ltd. (amount of a polar group: 80meq/kg)), and 570.0 parts of a mixed liquid of methyl ethyl ketone andcyclohexanone at 1:1 (mass ratio) as a solvent were mixed with respectto 100.0 parts of the abrasive (alumina powder) shown in Table 1, anddispersed in the presence of zirconia beads (bead diameter: 0.1 mm) by apaint shaker for the time (beads dispersion time) shown in Table 1.

After the dispersion, the dispersion liquid obtained by separating thedispersion liquid and the beads with a mesh was subjected to centrifugalseparation. The centrifugal separation was carried out using CS150GXLmanufactured by Koki Holdings Co., Ltd. (the rotor used is S100AT6manufactured by Koki Holdings Co., Ltd.) as a centrifugal separator atthe rotation speed (rotation per minute (rpm)) shown in Table 1 for thetime (centrifugal separation time) shown in Table 1. By this centrifugalseparation, particles having a relatively large particle size weresedimented, and particles having a relatively small particle size weredispersed in a supernatant.

After that, the supernatant was collected by decantation. This collectedliquid is called an “abrasive liquid A”.

Preparation of Abrasive Liquids B and C

An abrasive liquid B and an abrasive liquid C were prepared in the samemanner as in the preparation of the abrasive liquid A except thatvarious items were changed as shown in Table 1.

TABLE 1 Abrasive Abrasive Abrasive liquid A liquid B liquid CPreparation Abrasive product name Hit80 Hit70 Hit70 of abrasive(manufactured by Sumitomo liquid Chemical Co., Ltd.) BET specificsurface area 30 20 20 of abrasive (m²/g) Content of abrasive liquid 3.0parts 3.0 parts None dispersing agent (2,3-dihydroxynaphthalene) Beadsdispersion time 360 min 180 min 60 min Centrifugal Rotation speed 5500rpm 3500 rpm 1000 rpm separation Centrifugal 4 min 4 min 4 minseparation time

Preparation of Filler Liquid

Preparation of Filler Liquid D

Polyethyleneimine having the amount shown in Table 2, stearic acidhaving the amount shown in Table 2, and 570.0 parts of a mixed liquid ofmethyl ethyl ketone and cyclohexanone at 1:1 (mass ratio) as a solventwere mixed with respect to 100.0 parts of the filler (carbon black)shown in Table 2, and dispersed in the presence of zirconia beads (beaddiameter: 0.1 mm) by a paint shaker for the time (beads dispersion time)shown in Table 2.

After the dispersion, the dispersion liquid obtained by separating thedispersion liquid and the beads with a mesh was subjected to centrifugalseparation. The centrifugal separation was carried out using CS150GXLmanufactured by Koki Holdings Co., Ltd. (the rotor used is S100AT6manufactured by Koki Holdings Co., Ltd.) as a centrifugal separator atthe rotation speed (rotation per minute (rpm)) shown in Table 2 for thetime (centrifugal separation time) shown in Table 2. By this centrifugalseparation, particles having a relatively large particle size weresedimented, and particles having a relatively small particle size weredispersed in a supernatant.

After that, the supernatant was collected by decantation. This collectedliquid is called a “filler liquid D”.

The polyethyleneimine is a commercially available product(number-average molecular weight of 600) manufactured by Nippon ShokubaiCo., Ltd.

Preparation of Filler Liquids E to G

Filler liquids E to G were prepared in the same manner as in thepreparation of the filler liquid D except that various items werechanged as shown in Table 2.

TABLE 2 Filler Filler Filler Filler liquid D liquid E liquid F liquid GPreparation Filler product name (carbon black Asahi #50 Asahi #50 Asahi#50 Asahi #50 of filler manufactured by Asahi Carbon Co., Ltd.) liquidBET specific surface area of filler (m²/g) 23 23 23 23 Polyethyleneimine1.0 part 1.0 part 1.0 part None Stearic acid 2.0 parts 2.0 parts 2.0parts None Beads dispersion time 360 min 60 min 10 min 180 minCentrifugal Rotation speed 5500 rpm 3500 rpm 1000 rpm 5500 rpmseparation Centrifugal 4 min 4 min 4 min 4 min separation time

Example 1

Preparation of Magnetic Layer Forming Composition

Magnetic Liquid

Ferromagnetic powder: 100.0 parts

-   -   Hexagonal barium ferrite powder (“BaFe” in Table 3) having an        average particle size (average plate diameter) of 21 nm

Oleic acid: 2.0 parts

Vinyl chloride copolymer (MR-104 manufactured by Zeon Corporation): 10.0parts

SO₃Na group-containing polyurethane resin: 4.0 parts

-   -   (weight-average molecular weight: 70,000, SO₃Na group: 0.07        meq/g)

Amine-based polymer (DISPERBYK-102 manufactured by BYK-Chemie): 6.0parts

Methyl ethyl ketone: 150.0 parts

Cyclohexanone: 150.0 parts

Abrasive Liquid

Use the abrasive liquid shown in Table 3 so that the amount of abrasivein the abrasive liquid is the amount shown in Table 3

Filler Liquid

Use the filler liquid shown in Table 3 so that the amount of filler inthe filler liquid is the amount shown in Table 3

Other Components

Stearic acid: 3.0 parts

Stearic acid amide: 0.3 parts

Butyl stearate: 6.0 parts

Methyl ethyl ketone: 110.0 parts

Cyclohexanone: 110.0 parts

Polyisocyanate (CORONATE (registered trademark) L manufactured by TosohCorporation): 3.0 parts

Preparation Method

Various components of the above magnetic liquid were dispersed usingzirconia beads (first dispersion beads, density of 6.0 g/cm³) having abead diameter of 0.5 mm by a batch type vertical sand mill for 24 hours(first stage), and then filtered using a filter having a pore diameterof 0.5 μm. Thereby, a dispersion liquid A was prepared. The zirconiabeads were used in an amount of 10 times the mass of the ferromagneticpowder on a mass basis.

After that, the dispersion liquid A was dispersed using diamond beads(second dispersion beads, density of 3.5 g/cm³) having a bead diameterof 500 nm by a batch type vertical sand mill for 1 hour (second stage),and a dispersion liquid (dispersion liquid B) in which the diamond beadswere separated using a centrifugal separator was prepared. The diamondbeads were used in an amount of 10 times the mass of the ferromagneticpowder on a mass basis.

The dispersion liquid B, the abrasive liquid, the filler liquid, and theother components described above were put into a dissolver stirrer, andstirred for 360 minutes at a circumferential speed of 10 m/sec. Afterthat, an ultrasonic dispersion treatment was performed at a flow rate of7.5 kg/min for 60 minutes by a flow type ultrasonic dispersing device,and then the obtained liquid was filtered three times through a filterhaving a pore diameter of 0.3 μm. Thereby, a magnetic layer formingcomposition was prepared.

Preparation of Non-Magnetic Layer Forming Composition

Various components of non-magnetic layer forming composition describedbelow were dispersed using zirconia beads having a bead diameter of 0.1mm by a batch type vertical sand mill for 24 hours, and then filteredusing a filter having a pore diameter of 0.5 μm. Thereby, thenon-magnetic layer forming composition was prepared.

Non-Magnetic Inorganic Powder

α-iron oxide: 100.0 parts

-   -   (average particle size: 10 nm, BET specific surface area: 75        m²/g)

Carbon black: 25.0 parts

-   -   (average particle size: 20 nm)

SO₃Na group-containing polyurethane resin: 18.0 parts

-   -   (weight-average molecular weight: 70,000, SO₃Na group content:        0.2 meq/g)

Stearic acid: 1.0 part

Cyclohexanone: 300.0 parts

Methyl ethyl ketone: 300.0 parts

Preparation of Back Coating Layer Forming Composition

Components other than a lubricant (stearic acid and butyl stearate),polyisocyanate and 200.0 parts of cyclohexanone among the variouscomponents of back coating layer forming composition described belowwere kneaded and diluted by an open kneader, and then subjected to adispersion treatment of 12 passes using a horizontal beads milldispersing device and zirconia beads having a bead diameter of 1 mm, bysetting a bead filling percentage to 80 volume %, a circumferentialspeed of a rotor distal end to 10 m/sec, and a retention time per 1 passto 2 minutes. After that, the remaining components were added andstirred by a dissolver, and the obtained dispersion liquid was filteredusing a filter having a pore diameter of 1 μm. Thereby, a back coatinglayer forming composition was prepared.

Non-Magnetic Inorganic Powder

α-iron oxide: 80.0 parts

-   -   (average particle size: 0.15 μm, BET specific surface area: 52        m²/g)

Carbon black: 20.0 parts

-   -   (average particle size: 20 nm)

Vinyl chloride copolymer: 13.0 parts

sulfonate group-containing polyurethane resin: 6.0 parts

Phenylphosphonic acid: 3.0 parts

Cyclohexanone: 155.0 parts

Methyl ethyl ketone: 155.0 parts

Stearic acid: 3.0 parts

Butyl stearate: 3.0 parts

Polyisocyanate: 5.0 parts

Cyclohexanone: 200.0 parts

Manufacture of Magnetic Tape and Magnetic Tape Cartridge Group

The non-magnetic layer forming composition prepared in the above sectionwas applied onto a surface of a polyethylene naphthalate support havinga thickness of 4.2 μm and was dried so that the thickness after dryingis a thickness of 0.7 μm, and thus a non-magnetic layer was formed.

Next, the magnetic layer forming composition prepared in the abovesection was applied onto the non-magnetic layer so that the thicknessafter drying is 0.1 μm, and thus a coating layer was formed.

After that, while this coating layer of the magnetic layer formingcomposition is in a wet state, a vertical orientation treatment wasperformed by applying a magnetic field of a magnetic field intensity of0.3 T in a direction perpendicular to a surface of the coating layer,and then the surface of the coating layer was dried. Thereby, a magneticlayer was formed.

After that, the back coating layer forming composition prepared in theabove section was applied onto a surface of the support opposite to thesurface on which the non-magnetic layer and the magnetic layer areformed and was dried so that the thickness after drying is 0.3 μm, andthus, a back coating layer was formed.

After that, a surface smoothing treatment (calendering treatment) wasperformed using a calender roll formed of only metal rolls at a speed of100 m/min, a linear pressure of 300 kg/cm, and a calender temperature of90° C. (surface temperature of calender roll).

After that, a heat treatment was performed for 36 hours in anenvironment of an atmosphere temperature of 70° C., and then a longmagnetic tape original roll was slit to have ½ inches width to obtain amagnetic tape. A servo signal was recorded on the magnetic layer of theobtained magnetic tape by a commercially available servo writer toobtain a magnetic tape having a servo pattern (timing-based servopattern) arranged according to a linear tape-open (LTO) ultrium format.The obtained magnetic tape (tape length: 960 m) was accommodated in asingle reel type magnetic tape cartridge.

The above processes were repeated to manufacture a total of more than200 rolls of magnetic tape cartridges (magnetic tape cartridge groups).

It could be confirmed by the following method that the magnetic layer ofthe magnetic tape includes the compound including the ammonium saltstructure of the alkyl ester anion represented by Formula 1, which isformed of polyethyleneimine and stearic acid.

A sample is cut out from the magnetic tape, and X-ray photoelectronspectroscopy analysis is performed on the magnetic layer surface(measurement area: 300 μm×700 μm) using an ESCA device. Specifically,the wide scanning measurement is performed by the ESCA device under thefollowing measurement conditions. In the measurement results, peaks areconfirmed at a binding energy position of an ester anion and a bindingenergy position of an ammonium cation.

Device: AXIS-ULTRA manufactured by Shimadzu Corporation

Excited X-ray source: monochromatic Al—Kα ray

Scanning range: 0 to 1,200 eV

Pass energy: 160 eV

Energy resolution: 1 eV/step

Take-in time: 100 ms/step

Accumulation number 5

In addition, a sample piece having a length of 3 cm is cut out from themagnetic tape, and the attenuated total reflection-fouriertransform-infrared spectrometer (ATR-FT-IR) measurement (reflectionmethod) is performed on the magnetic layer surface. In the measurementresults, an absorption is confirmed at the wave number (1540 cm⁻¹ or1430 cm⁻¹) corresponding to an absorption of COO⁻ and the wave number(2400 cm) corresponding to an absorption of an ammonium cation.

Examples 2 to 20 and Comparative Examples 1 to 18

A magnetic tape cartridge group was manufactured in the same manner asin Example 1 except that various items were changed as shown in Table 3.

Example 21

A magnetic tape cartridge group was manufactured in the same manner asin Example 3 except that hexagonal strontium ferrite powder (“SrFe1” inTable 3) manufactured as follows was used as the ferromagnetic powder.

1707 g of SrCO₃, 687 g of H₃BO₃, 1120 g of Fe₂O₃, 45 g of Al(OH)₃, 24 gof BaCO₃, 13 g of CaCO₃, and 235 g of Nd₂O₃ were weighed and mixed by amixer to obtain a raw material mixture.

The obtained raw material mixture was melted in a platinum crucible at amelting temperature of 1390° C., and a hot water outlet provided at abottom of the platinum crucible was heated while stirring a melt, andthe melt was discharged in a rod shape at about 6 g/sec. Hot water wasrolled and quenched by a water-cooled twin roller to manufacture anamorphous body.

280 g of the manufactured amorphous body was charged into an electricfurnace, was heated to 635° C. (crystallization temperature) at aheating rate of 3.5° C./min, and was kept at the same temperature for 5hours to precipitate (crystallize) hexagonal strontium ferriteparticles.

Next, a crystallized product obtained above including hexagonalstrontium ferrite particles was coarsely pulverized in a mortar, and1000 g of zirconia beads having a particle diameter of 1 mm and 800 mLof an acetic acid aqueous solution of 1% concentration were added to thecrystallized product in a glass bottle, to be dispersed by a paintshaker for 3 hours. Thereafter, the obtained dispersion liquid wasseparated from the beads, to be put in a stainless beaker. Thedispersion liquid was statically left at a liquid temperature of 100° C.for 3 hours and subjected to a dissolving process of a glass component,and then the crystallized product was sedimented by a centrifugalseparator to be washed by repeatedly performing decantation and wasdried in a heating furnace at an internal temperature of the furnace of110° C. for 6 hours to obtain hexagonal strontium ferrite powder.

The hexagonal strontium ferrite powder obtained above had an averageparticle size of 18 nm, an activation volume of 902 nm³, an anisotropyconstant Ku of 2.2×10⁵ J/m³, and a mass magnetization as of 49 A·m²/kg.

12 mg of sample powder was taken from the hexagonal strontium ferritepowder obtained above, elemental analysis of the filtrated solutionobtained by partially dissolving this sample powder under dissolutionconditions exemplified above was performed by an ICP analyzer, and asurface layer portion content of a neodymium atom was determined.

Separately, 12 mg of sample powder was taken from the hexagonalstrontium ferrite powder obtained above, elemental analysis of thefiltrated solution obtained by totally dissolving this sample powderunder dissolution conditions exemplified above was performed by an ICPanalyzer, and a bulk content of a neodymium atom was determined.

A content (bulk content) of a neodymium atom with respect to 100 at % ofan iron atom in the hexagonal strontium ferrite powder obtained abovewas 2.9 at %. A surface layer portion content of a neodymium atom was8.0 at %. It was confirmed that a ratio between a surface layer portioncontent and a bulk content, that is, “surface layer portion content/bulkcontent” was 2.8, and a neodymium atom was unevenly distributed in asurface layer of a particle.

The fact that the powder obtained above shows a crystal structure ofhexagonal ferrite was confirmed by performing scanning with CuKα raysunder conditions of a voltage of 45 kV and an intensity of 40 mA andmeasuring an X-ray diffraction pattern under the following conditions(X-ray diffraction analysis). The powder obtained above showed a crystalstructure of hexagonal ferrite of a magnetoplumbite type (M type). Acrystal phase detected by X-ray diffraction analysis was a single phaseof a magnetoplumbite type.

PANalytical X'Pert Pro diffractometer, PIXcel detector

Soller slit of incident beam and diffracted beam: 0.017 radians

Fixed angle of dispersion slit: ¼ degrees

Mask: 10 mm

Anti-scattering slit: ¼ degrees

Measurement mode: continuous

Measurement time per stage: 3 seconds

Measurement speed: 0.017 degrees per second

Measurement step: 0.05 degrees

Example 22

A magnetic tape cartridge group was manufactured in the same manner asin Example 3 except that hexagonal strontium ferrite powder (“SrFe2” inTable 3) manufactured as follows was used as the ferromagnetic powder.

1725 g of SrCO₃, 666 g of H₃BO₃, 1332 g of Fe₂O₃, 52 g of Al(OH)₃, 34 gof CaCO₃, and 141 g of BaCO₃ were weighed and mixed by a mixer to obtaina raw material mixture.

The obtained raw material mixture was dissolved in a platinum crucibleat a melting temperature of 1380° C., and a hot water outlet provided ata bottom of the platinum crucible was heated while stirring a melt, andthe melt was discharged in a rod shape at about 6 g/sec. Hot water wasrolled and quenched by a water-cooled twin roller to manufacture anamorphous body.

280 g of the obtained amorphous body was charged into an electricfurnace, was heated to 645° C. (crystallization temperature), and waskept at the same temperature for 5 hours to precipitate (crystallize)hexagonal strontium ferrite particles.

Next, a crystallized product obtained above including hexagonalstrontium ferrite particles was coarsely pulverized in a mortar, and1000 g of zirconia beads having a particle diameter of 1 mm and 800 mLof an acetic acid aqueous solution of 1% concentration were added to thecrystallized product in a glass bottle, to be dispersed by a paintshaker for 3 hours. Thereafter, the obtained dispersion liquid wasseparated from the beads, to be put in a stainless beaker. Thedispersion liquid was statically left at a liquid temperature of 100° C.for 3 hours and subjected to a dissolving process of a glass component,and then the crystallized product was sedimented by a centrifugalseparator to be washed by repeatedly performing decantation and wasdried in a heating furnace at an internal temperature of the furnace of110° C. for 6 hours to obtain hexagonal strontium ferrite powder.

The obtained hexagonal strontium ferrite powder had an average particlesize of 19 nm, an activation volume of 1102 nm³, an anisotropy constantKu of 2.0×10⁵ J/m³, and a mass magnetization as of 50 A·m²/kg.

Example 23

A magnetic tape cartridge group was manufactured in the same manner asin Example 3 except that ε-iron oxide powder (“ε-iron oxide” in Table 3)manufactured as follows was used as the ferromagnetic powder.

8.3 g of iron(III) nitrate nonahydrate, 1.3 g of gallium(III) nitrateoctahydrate, 190 mg of cobalt(II) nitrate hexahydrate, 150 mg oftitanium(IV) sulfate, and 1.5 g of polyvinylpyrrolidone (PVP) weredissolved in 90 g of pure water, and while the dissolved product wasstirred using a magnetic stirrer, 4.0 g of an aqueous ammonia solutionhaving a concentration of 25% was added to the dissolved product under acondition of an atmosphere temperature of 25° C. in an air atmosphere,and the dissolved product was stirred for 2 hours while maintaining atemperature condition of the atmosphere temperature of 25° C. A citricacid aqueous solution obtained by dissolving 1 g of citric acid in 9 gof pure water was added to the obtained solution, and the mixture wasstirred for 1 hour. The powder sedimented after stirring was collectedby centrifugal separation, was washed with pure water, and was dried ina heating furnace at an internal temperature of the furnace of 80° C.

800 g of pure water was added to the dried powder, and the powder wasdispersed again in water to obtain dispersion liquid. The obtaineddispersion liquid was heated to a liquid temperature of 50° C., and 40 gof an aqueous ammonia solution having a concentration of 25% wasdropwise added with stirring. After stirring for 1 hour whilemaintaining the temperature at 50° C., 14 mL of tetraethoxysilane (TEOS)was dropwise added and was stirred for 24 hours. Powder sedimented byadding 50 g of ammonium sulfate to the obtained reaction solution wascollected by centrifugal separation, was washed with pure water, and wasdried in a heating furnace at an internal temperature of the furnace of80° C. for 24 hours to obtain a ferromagnetic powder precursor.

The obtained ferromagnetic powder precursor was loaded into a heatingfurnace at an internal temperature of the furnace of 1000° C. in an airatmosphere and was heat-treated for 4 hours.

The heat-treated ferromagnetic powder precursor was put into an aqueoussolution of 4 mol/L sodium hydroxide (NaOH), and the liquid temperaturewas maintained at 70° C. and was stirred for 24 hours, whereby a silicicacid compound as an impurity was removed from the heat-treatedferromagnetic powder precursor.

Thereafter, the ferromagnetic powder from which the silicic acidcompound was removed was collected by centrifugal separation, and waswashed with pure water to obtain a ferromagnetic powder.

The composition of the obtained ferromagnetic powder that was checked byhigh-frequency inductively coupled plasma-optical emission spectrometry(ICP-OES) has Ga, Co, and a Ti substitution type ε-iron oxide(ε-Ga_(0.28)Co_(0.05)Ti_(0.05)Fe_(1.62)O₃). In addition, X-raydiffraction analysis is performed under the same condition as describedabove for the hexagonal strontium ferrite powder SrFe1, and from a peakof an X-ray diffraction pattern, it is checked that the obtainedferromagnetic powder does not include α-phase and γ-phase crystalstructures, and has a single-phase and ε-phase crystal structure (ε-ironoxide type crystal structure).

The obtained ε-iron oxide powder had an average particle size of 12 nm,an activation volume of 746 nm³, an anisotropy constant Ku of 1.2×10⁵J/m³, and a mass magnetization as of 16 A·m²/kg.

An activation volume and an anisotropy constant Ku of the abovehexagonal strontium ferrite powder and ε-iron oxide powder are valuesobtained by the method described above using a vibrating samplemagnetometer (manufactured by Toei Industry Co., Ltd.) for eachferromagnetic powder.

A mass magnetization σs is a value measured at a magnetic fieldintensity of 1194 kA/m (15 kOe) using a vibrating sample magnetometer(manufactured by Toei Industry Co., Ltd.).

TABLE 3 Ferromagnetic Abrasive liquid Filler liquid powder A B C D E F GExample 1 BaFe 6.0 parts 2.5 parts 3.0 parts 1.3 parts 1.7 parts 0.3parts 0.0 parts Example 2 BaFe 2.0 parts 2.5 parts 3.0 parts 1.3 parts1.7 parts 0.3 parts 0.0 parts Example 3 BaFe 6.0 parts 2.5 parts 3.0parts 0.1 parts 1.7 parts 0.3 parts 0.0 parts Example 4 BaFe 6.0 parts0.7 parts 3.0 parts 1.3 parts 0.1 parts 0.3 parts 0.0 parts Example 5BaFe 6.0 parts 2.5 parts 1.0 part 0.1 parts 0.1 parts 0.3 parts 0.0parts Example 6 BaFe 6.0 parts 0.7 parts 3.0 parts 1.3 parts 0.1 parts0.0 parts 0.0 parts Example 7 BaFe 6.0 parts 0.7 parts 1.0 part 1.3parts 1.7 parts 0.0 parts 0.0 parts Example 8 BaFe 4.0 parts 1.6 parts2.0 parts 1.3 parts 1.7 parts 0.0 parts 0.0 parts Example 9 BaFe 6.0parts 2.5 parts 1.0 part 0.5 parts 0.7 parts 0.1 parts 0.0 parts Example10 BaFe 4.0 parts 1.6 parts 2.0 parts 0.5 parts 0.7 parts 0.1 parts 0.0parts Example 11 BaFe 4.0 parts 0.7 parts 2.0 parts 0.1 parts 0.1 parts0.1 parts 0.0 parts Example 12 BaFe 6.0 parts 1.6 parts 1.0 part 0.1parts 0.7 parts 0.3 parts 0.0 parts Example 13 BaFe 2.0 parts 2.5 parts3.0 parts 0.1 parts 0.1 parts 0.3 parts 0.0 parts Example 14 BaFe 2.0parts 0.7 parts 1.0 part 1.3 parts 1.7 parts 0.3 parts 0.0 parts Example15 BaFe 6.0 parts 2.5 parts 3.0 parts 0.1 parts 0.1 parts 0.0 parts 0.0parts Example 16 BaFe 2.0 parts 0.7 parts 1.0 part 1.3 parts 0.1 parts0.3 parts 0.0 parts Example 17 BaFe 6.0 parts 0.7 parts 3.0 parts 0.1parts 0.1 parts 0.0 parts 0.0 parts Example 18 BaFe 6.0 parts 0.7 parts1.0 part 1.3 parts 0.1 parts 0.0 parts 0.0 parts Example 19 BaFe 2.0parts 0.7 parts 3.0 parts 0.1 parts 0.1 parts 0.3 parts 0.0 partsExample 20 BaFe 2.0 parts 0.7 parts 1.0 part 0.1 parts 0.1 parts 0.0parts 0.0 parts Example 21 SrFe1 6.0 parts 2.5 parts 3.0 parts 0.1 parts1.7 parts 0.3 parts 0.0 parts Example 22 SrFe2 6.0 parts 2.5 parts 3.0parts 0.1 parts 1.7 parts 0.3 parts 0.0 parts Example 23 ε-iron oxide6.0 parts 2.5 parts 3.0 parts 0.1 parts 1.7 parts 0.3 parts 0.0 partsComparative BaFe 1.6 parts 3.0 parts 1.0 part 0.0 parts 0.0 parts 0.0parts 2.0 parts Example 1 Comparative BaFe 4.0 parts 1.6 parts 5.0 parts0.0 parts 0.7 parts 0.1 parts 0.0 parts Example 2 Comparative BaFe 6.4parts 1.6 parts 0.5 parts 0.5 parts 0.7 parts 0.4 parts 0.0 partsExample 3 Comparative BaFe 4.0 parts 1.6 parts 5.0 parts 0.5 parts 0.7parts 0.4 parts 0.0 parts Example 4 Comparative BaFe 6.4 parts 1.6 parts0.5 parts 0.0 parts 0.7 parts 0.6 parts 0.0 parts Example 5 ComparativeBaFe 6.4 parts 1.6 parts 2.0 parts 0.0 parts 0.0 parts 0.0 parts 2.4parts Example 6 Comparative BaFe 4.0 parts 3.0 parts 2.0 parts 0.0 parts0.0 parts 0.0 parts 2.4 parts Example 7 Comparative BaFe 4.0 parts 3.0parts 5.0 parts 0.0 parts 0.0 parts 0.0 parts 2.4 parts Example 8Comparative BaFe 1.6 parts 1.6 parts 2.0 parts 0.0 parts 0.0 parts 0.0parts 0.8 parts Example 9 Comparative BaFe 6.4 parts 0.5 parts 2.0 parts0.0 parts 0.0 parts 0.0 parts 0.8 parts Example 10 Comparative BaFe 6.4parts 1.6 parts 5.0 parts 0.0 parts 0.0 parts 0.0 parts 0.8 partsExample 11 Comparative BaFe 4.0 parts 0.5 parts 2.0 parts 0.0 parts 0.0parts 0.0 parts 2.4 parts Example 12 Comparative BaFe 8.0 parts 1.6parts 2.0 parts 0.5 parts 0.7 parts 0.1 parts 0.0 parts Example 13Comparative BaFe 4.0 parts 3.0 parts 2.0 parts 0.5 parts 0.7 parts 0.1parts 0.0 parts Example 14 Comparative BaFe 4.0 parts 1.6 parts 5.0parts 0.5 parts 0.7 parts 0.1 parts 0.0 parts Example 15 ComparativeBaFe 4.0 parts 1.6 parts 2.0 parts 0.0 parts 0.0 parts 0.0 parts 0.8parts Example 16 Comparative BaFe 4.0 parts 1.6 parts 2.0 parts 0.5parts 2.3 parts 0.1 parts 0.0 parts Example 17 Comparative BaFe 4.0parts 1.6 parts 2.0 parts 0.5 parts 0.7 parts 0.6 parts 0.0 partsExample 18

Evaluation of Magnetic Tape

One roll of the magnetic tape cartridge was extracted from each magnetictape cartridge group of Examples and Comparative Examples, and physicalproperties of the magnetic tape accommodated in the extracted magnetictape cartridge were evaluated by the following method.

Number Distribution A and Number Distribution B

Using an FE-SEM S4800 manufactured by Hitachi, Ltd. as a scanningelectron microscope (FE-SEM), the number distribution A and the numberdistribution B of the magnetic layer surface of each magnetic tape wereobtained by the following method.

Number Distribution A

A secondary electron image of the magnetic layer surface of the magneticrecording medium to be measured is captured using a scanning electronmicroscope (FE-SEM). As imaging conditions, an acceleration voltage is 5kV, an operating distance is 5 mm, and an imaging magnification is10,000. In imaging, a non-imaging region on the magnetic layer surfaceis selected, focus adjustment is performed under the imaging conditions,and a secondary electron image is captured. A part (micron bar, crossmark, or the like) for displaying the size and the like is erased fromthe captured image, and a secondary electron image having the number ofpixels of 960 pixels×1280 pixels is acquired.

The above operation is performed 100 times at different positions on themagnetic layer surface of the magnetic recording medium to be measured.

The secondary electron image thus acquired is taken into imageprocessing software (free software ImageJ), and is binarized by thefollowing procedure.

For a threshold value for binarizing the secondary electron imageacquired above, a lower limit is set to 210 gradations and an upperlimit is set to 255 gradations, and the binarization processing isexecuted based on these two threshold values. After the binarizationprocessing, in the image analysis software (free software ImageJ), noisecut processing Despeckle is selected to remove the noise component.

For the binarized image thus obtained, the number of bright regions(that is, white parts) and the area of each bright region are obtainedby the image analysis software (free software ImageJ). From the area Aof the bright region obtained here, an equivalent circle diameter L ofeach bright region is calculated by (A/π){circumflex over ( )}(½)×2=L.

The above processes are performed on the binarized image (100 images)obtained above. From the above, the number distribution A is obtained.

Number Distribution B

A secondary electron image of the magnetic layer surface of the magneticrecording medium to be measured is captured using a scanning electronmicroscope (FE-SEM). As imaging conditions, an acceleration voltage is 2kV, an operating distance is 5 mm, and an imaging magnification is10,000. In imaging, a non-imaging region on the magnetic layer surfaceis selected, focus adjustment is performed under the imaging conditions,and a secondary electron image is captured. A part (micron bar, crossmark, or the like) for displaying the size and the like is erased fromthe captured image, and a secondary electron image having the number ofpixels of 960 pixels×1280 pixels is acquired.

The above operation is performed 100 times at different positions on themagnetic layer surface of the magnetic recording medium to be measured.

The secondary electron image thus acquired is taken into imageprocessing software (free software ImageJ), and is binarized by thefollowing procedure.

For a threshold value for binarizing the secondary electron imageacquired above, a lower limit is set to 0 gradation and an upper limitis set to 75 gradations, and the binarization processing is executedbased on these two threshold values. After the binarization processing,in the image analysis software (free software ImageJ), noise cutprocessing Despeckle is selected to remove the noise component.

For the binarized image thus obtained, the number of dark regions (thatis, black parts) and the area of each dark region are obtained by theimage analysis software (free software ImageJ). From the area A of thedark region obtained here, an equivalent circle diameter L of each darkregion is calculated by (A/π){circumflex over ( )}(½)×2=L.

The above processes are performed on the binarized image (100 images)obtained above. From the above, the number distribution B is obtained.

Total Thickness of Magnetic Tape (Tape Thickness)

Ten tape samples (5 cm in length) were cut out from any part of themagnetic tape, and these tape samples were stacked to measure thethickness. The thickness was measured using a digital thickness gauge ofMillimar 1240 compact amplifier and Millimar 1301 induction probemanufactured by Mahr Inc. A value (thickness per tape sample) obtainedby dividing the measured thickness by 1/10 was set as the tapethickness. For each magnetic tape, the tape thickness was 5.3 μm.

Evaluation of Magnetic Tape Cartridge Group

GTT Slope α

A total of 200 rolls of the magnetic tape cartridges were randomlyextracted from each magnetic tape cartridge group of Examples andComparative Examples, and for these magnetic tape cartridges, the GTTslope α was obtained in an environment of an atmosphere temperature of21° C. and a relative humidity of 50% by the method described aboveusing an LTO8 drive.

Reproduction Quality in GTT

The number of channels means the number of tracks to be reproduced atthe same time, and the number of channels in the LTO8 drive is 32channels. During reproduction, in a case where reproduction failureoccurs in some of the tracks to be reproduced at the same time,reproduction error information is displayed on the drive.

In the evaluation of the GTT slope α, in the reproduction of therecorded data in a total of 200 rolls of the magnetic tape cartridges,the evaluation result was set to “A” in a case where the reproductionerror information was not displayed (that is, in a case where all thetracks to be reproduced at the same time could be reproduced withoutoccurrence of reproduction failure), and the evaluation result was setto “B” in a case where the reproduction error information was displayed.

Based on the above evaluation standard, the reproduction quality in GTTin an environment of an atmosphere temperature of 21° C. and a relativehumidity of 50% was evaluated.

The above results are shown in Table 4 (Table 4-1 and Table 4-2).

TABLE 4-1 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or GTT Reproduction more and 50 more and 100 101 nm more and50 more and 100 101 nm slope α quality nm or less nm or less or more nmor less nm or less or more (dB/decade) in GTT Example 1 30000 25000 300025000 5000 200 0.3 A Example 2 10000 25000 3000 25000 5000 200 0.2 AExample 3 30000 25000 3000 1000 5000 200 0.1 A Example 4 30000 7000 300025000 200 200 0.1 A Example 5 30000 25000 1000 1000 200 200 0.1 AExample 6 30000 7000 3000 25000 200 0 0.3 A Example 7 30000 7000 100025000 5000 0 0.2 A Example 8 20000 16000 2000 25000 5000 0 0.1 A Example9 30000 25000 1000 10000 2000 100 0.1 A Example 10 20000 16000 200010000 2000 100 0.1 A Example 11 20000 7000 2000 1000 200 100 0.1 AExample 12 30000 16000 1000 1000 2000 200 0.1 A Example 13 10000 250003000 1000 200 200 0.2 A Example 14 10000 7000 1000 25000 5000 200 0.3 AExample 15 30000 25000 3000 1000 200 0 0.2 A Example 16 10000 7000 100025000 200 200 0.1 A Example 17 30000 7000 3000 10000 200 0 0.2 A Example18 30000 7000 1000 25000 200 0 0.1 A Example 19 10000 7000 3000 1000 200200 0.2 A Example 20 10000 7000 1000 1000 200 0 0.3 A Example 21 3000025000 3000 1000 5000 200 0.1 A Example 22 30000 25000 3000 1000 5000 2000.1 A Example 23 30000 25000 3000 1000 5000 200 0.1 A

TABLE 4-2 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or GTT Reproduction more and 50 more and 100 101 nm more and50 more and 100 101 nm slope α quality nm or less nm or less or more nmor less nm or less or more (dB/decade) in GTT Comparative 8000 300001000 0 7000 200 0.8 B Example 1 Comparative 20000 16000 5000 600 2000100 1.1 B Example 2 Comparative 32000 16000 500 10000 2000 280 0.9 BExample 3 Comparative 20000 16000 5000 10000 2000 280 1.3 B Example 4Comparative 32000 16000 500 600 2000 450 1.6 B Example 5 Comparative32000 16000 2000 0 7000 240 1.0 B Example 6 Comparative 20000 30000 20000 7000 240 1.9 B Example 7 Comparative 20000 30000 5000 0 7000 240 2.0 BExample 8 Comparative 8000 16000 2000 0 2000 80 1.8 B Example 9Comparative 32000 5000 2000 0 2000 80 1.5 B Example 10 Comparative 3200016000 5000 0 2000 80 2.8 B Example 11 Comparative 20000 5000 2000 0 7000240 3.0 B Example 12 Comparative 40000 16000 2000 10000 2000 100 0.8 BExample 13 Comparative 20000 30000 2000 10000 2000 100 1.0 B Example 14Comparative 20000 16000 5000 10000 2000 100 1.5 B Example 15 Comparative20000 16000 2000 0 2000 80 1.6 B Example 16 Comparative 20000 16000 200010000 7000 100 0.9 B Example 17 Comparative 20000 16000 2000 10000 2000450 1.2 B Example 18

Examples 24 to 54 and Comparative Examples 19 to 37

A magnetic tape was manufactured in the same manner as in Example 1except that various items were changed as shown in Table 5, and theelectromagnetic conversion characteristics (SNR) of the manufacturedmagnetic tape were evaluated by the following method.

In Table 5, the vertical orientation treatment was not performed forExamples and Comparative Examples described as “OT” in the column of“magnetic field intensity during vertical orientation”.

Evaluation Method of Electromagnetic Conversion Characteristics

In an environment of an atmosphere temperature of 23° C.±1° C. and arelative humidity of 50%, a magnetic tape was attached to a ½ inchesreel tester to which a recording head and a reproducing head were fixed,and recording and reproducing of data were performed at a relative speedof 4 m/sec between the recording head or the reproducing head and themagnetic tape during recording and reproducing.

As the recording head, for Examples and Comparative Examples describedas “both sides” in the column of “recording element film formation” inTable 5, a magnetic head was used comprising an inductive recordingelement in which magnetic poles on both sides of the recording element(write gap length of 150 nm, track width of 3.0 μm) made of permalloy(Fe of 45%. Ni of 55% in at %) were sputtered with a CoFeNi alloy havinga thickness of 100 nm at tip portions on both sides facing each otherwith a write gap between the magnetic poles. For Examples andComparative Examples described as “one side” in the column of “recordingelement film formation” in Table 5, a magnetic head comprising arecording element in which the CoFeNi alloy was formed only on onemagnetic pole (second magnetic pole (trailing side)) was used as therecording head.

In each of Examples and Comparative Examples, a commercially availableTMR head (element width of 1,000 nm) was used as the reproducing head.Recording was performed at a linear recording density of 300 kfci, thereproduction output during reproduction was measured, and the SNR wasobtained as a signal-to-noise-ratio (ratio between the reproductionoutput and noise). The SNR was calculated as a relative value where theSNR measured for Comparative Example 19 was 0.0 dB. The evaluationresults are shown in Table 6 (Table 6-1 and Table 6-2).

The vertical squareness ratio shown in Table 6 is a value obtained foreach magnetic tape by the method described above using a vibratingsample magnetometer (manufactured by Toei Industry Co., Ltd.).

The number distribution A and the number distribution B shown in Table 6were obtained by the same method as in Example 1 and the like.

TABLE 5 Magnetic field intensity during Recording Abrasive liquid Fillerliquid vertical element film A B C D E F G orientation formation Example24 6.0 parts 2.5 parts 3.0 parts 1.3 parts 1.7 parts 0.3 parts 0.0 parts0.3 T Both sides Example 25 2.0 parts 2.5 parts 3.0 parts 1.3 parts 1.7parts 0.3 parts 0.0 parts 0.3 T Both sides Example 26 6.0 parts 2.5parts 3.0 parts 0.1 parts 1.7 parts 0.3 parts 0.0 parts 0.3 T Both sidesExample 27 6.0 parts 0.7 parts 3.0 parts 1.3 parts 0.1 parts 0.3 parts0.0 parts 0.3 T Both sides Example 28 6.0 parts 2.5 parts 1.0 part 0.1parts 0.1 parts 0.3 parts 0.0 parts 0.3 T Both sides Example 29 6.0parts 0.7 parts 3.0 parts 1.3 parts 0.1 parts 0.0 parts 0.0 parts 0.3 TBoth sides Example 30 6.0 parts 0.7 parts 1.0 part 1.3 parts 1.7 parts0.0 parts 0.0 parts 0.3 T Both sides Example 31 4.0 parts 1.6 parts 2.0parts 1.3 parts 1.7 parts 0.0 parts 0.0 parts 0.3 T Both sides Example32 6.0 parts 2.5 parts 1.0 part 0.5 parts 0.7 parts 0.1 parts 0.0 parts0.3 T Both sides Example 33 4.0 parts 1.6 parts 2.0 parts 0.5 parts 0.7parts 0.1 parts 0.0 parts 0.3 T Both sides Example 34 4.0 parts 0.7parts 2.0 parts 0.1 parts 0.1 parts 0.1 parts 0.0 parts 0.3 T Both sidesExample 35 6.0 parts 1.6 parts 1.0 part 0.1 parts 0.7 parts 0.3 parts0.0 parts 0.3 T Both sides Example 36 2.0 parts 2.5 parts 3.0 parts 0.1parts 0.1 parts 0.3 parts 0.0 parts 0.3 T Both sides Example 37 2.0parts 0.7 parts 1.0 part 1.3 parts 1.7 parts 0.3 parts 0.0 parts 0.3 TBoth sides Example 38 6.0 parts 2.5 parts 3.0 parts 0.1 parts 0.1 parts0.0 parts 0.0 parts 0.3 T Both sides Example 39 2.0 parts 0.7 parts 1.0part 1.3 parts 0.1 parts 0.3 parts 0.0 parts 0.3 T Both sides Example 406.0 parts 0.7 parts 3.0 parts 0.1 parts 0.1 parts 0.0 parts 0.0 parts0.3 T Both sides Example 41 6.0 parts 0.7 parts 1.0 part 1.3 parts 0.1parts 0.0 parts 0.0 parts 0.3 T Both sides Example 42 2.0 parts 0.7parts 3.0 parts 0.1 parts 0.1 parts 0.3 parts 0.0 parts 0.3 T Both sidesExample 43 2.0 parts 0.7 parts 1.0 part 0.1 parts 0.1 parts 0.0 parts0.0 parts 0.3 T Both sides Example 44 2.0 parts 0.7 parts 1.0 part 0.1parts 0.1 parts 0.0 parts 0.0 parts 0.5 T Both sides Example 45 2.0parts 0.7 parts 1.0 part 0.1 parts 0.1 parts 0.0 parts 0.0 parts 1.0 TBoth sides Example 46 6.0 parts 2.5 parts 3.0 parts 1.3 parts 1.7 parts0.3 parts 0.0 parts 0.5 T Both sides Example 47 6.0 parts 2.5 parts 3.0parts 1.3 parts 1.7 parts 0.3 parts 0.0 parts 1.0 T Both sides Example48 6.0 parts 0.7 parts 1.0 part 1.3 parts 1.7 parts 0.0 parts 0.0 parts0.5 T Both sides Example 49 6.0 parts 0.7 parts 1.0 part 1.3 parts 1.7parts 0.0 parts 0.0 parts 1.0 T Both sides Example 50 4.0 parts 1.6parts 2.0 parts 0.5 parts 0.7 parts 0.1 parts 0.0 parts 0.5 T Both sidesExample 51 4.0 parts 1.6 parts 2.0 parts 0.5 parts 0.7 parts 0.1 parts0.0 parts 1.0 T Both sides Example 52 0.6 parts 0.1 parts 2.0 parts 0.2parts 0.1 parts 0.0 parts 0.0 parts 0 T One side Example 53 2.0 parts2.5 parts 20.0 parts 0.6 parts 5.0 parts 0.3 parts 0.0 parts 0 T Oneside Example 54 1.6 parts 0.5 parts 4.0 parts 0.3 parts 1.0 part 0.1parts 0.0 parts 0 T One side Comparative 1.6 parts 3.0 parts 1.0 part0.0 parts 0.0 parts 0.0 parts 2.0 parts 0 T One side Example 19Comparative 4.0 parts 1.6 parts 5.0 parts 0.0 parts 0.7 parts 0.1 parts0.0 parts 0 T One side Example 20 Comparative 6.4 parts 1.6 parts 0.5parts 0.5 parts 0.7 parts 0.4 parts 0.0 parts 0 T One side Example 21Comparative 4.0 parts 1.6 parts 5.0 parts 0.5 parts 0.7 parts 0.4 parts0.0 parts 0 T One side Example 22 Comparative 6.4 parts 1.6 parts 0.5parts 0.0 parts 0.7 parts 0.6 parts 0.0 parts 0 T One side Example 23Comparative 6.4 parts 1.6 parts 2.0 parts 0.0 parts 0.0 parts 0.0 parts2.4 parts 0 T One side Example 24 Comparative 4.0 parts 3.0 parts 2.0parts 0.0 parts 0.0 parts 0.0 parts 2.4 parts 0 T One side Example 25Comparative 4.0 parts 3.0 parts 5.0 parts 0.0 parts 0.0 parts 0.0 parts2.4 parts 0 T One side Example 26 Comparative 1.6 parts 1.6 parts 2.0parts 0.0 parts 0.0 parts 0.0 parts 0.8 parts 0 T One side Example 27Comparative 6.4 parts 0.5 parts 2.0 parts 0.0 parts 0.0 parts 0.0 parts0.8 parts 0 T One side Example 28 Comparative 6.4 parts 1.6 parts 5.0parts 0.0 parts 0.0 parts 0.0 parts 0.8 parts 0 T One side Example 29Comparative 4.0 parts 0.5 parts 2.0 parts 0.0 parts 0.0 parts 0.0 parts2.4 parts 0 T One side Example 30 Comparative 1.6 parts 3.0 parts 6.7parts 0.0 parts 7.0 parts 0.3 parts 0.0 parts 0.3 T One side Example 31Comparative 6.4 parts 1.6 parts 3.3 parts 0.0 parts 2.0 parts 0.6 parts0.0 parts 0.3 T One side Example 32 Comparative 4.0 parts 0.5 parts 13.3parts 0.0 parts 0.0 parts 0.0 parts 3.0 parts 0.3 T One side Example 33Comparative 1.6 parts 3.0 parts 6.7 parts 0.0 parts 7.0 parts 0.3 parts0.0 parts 1.0 T One side Example 34 Comparative 1.6 parts 3.0 parts 6.7parts 0.0 parts 7.0 parts 0.3 parts 0.0 parts 0 T Both sides Example 35Comparative 1.6 parts 3.0 parts 6.7 parts 0.0 parts 7.0 parts 0.3 parts0.0 parts 0.3 T Both sides Example 36 Comparative 1.6 parts 3.0 parts6.7 parts 0.0 parts 7.0 parts 0.3 parts 0.0 parts 1.0 T Both sidesExample 37

TABLE 6-1 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or Vertical more and 50 more and 100 101 nm more and 50 moreand 100 101 nm squareness SNR nm or less nm or less or more nm or lessnm or less or more ratio (dB) Example 24 30000 25000 3000 25000 5000 2000.65 3.0 Example 25 10000 25000 3000 25000 5000 200 0.65 3.0 Example 2630000 25000 3000 1000 5000 200 0.65 3.0 Example 27 30000 7000 3000 25000200 200 0.65 3.0 Example 28 30000 25000 1000 1000 200 200 0.65 3.0Example 29 30000 7000 3000 25000 200 0 0.65 3.5 Example 30 30000 70001000 25000 5000 0 0.65 3.5 Example 31 20000 16000 2000 25000 5000 0 0.653.5 Example 32 30000 25000 1000 10000 2000 100 0.65 3.0 Example 33 2000016000 2000 10000 2000 100 0.65 3.0 Example 34 20000 7000 2000 1000 200100 0.65 3.0 Example 35 30000 16000 1000 1000 2000 200 0.65 3.0 Example36 10000 25000 3000 1000 200 200 0.65 3.0 Example 37 10000 7000 100025000 5000 200 0.65 3.0 Example 38 30000 25000 3000 1000 200 0 0.65 3.5Example 39 10000 7000 1000 25000 200 200 0.65 3.0 Example 40 30000 70003000 1000 200 0 0.65 3.5 Example 41 30000 7000 1000 25000 200 0 0.65 3.5Example 42 10000 7000 3000 1000 200 200 0.65 3.0 Example 43 10000 70001000 1000 200 0 0.65 3.5 Example 44 10000 7000 1000 1000 200 0 0.70 5.0Example 45 10000 7000 1000 1000 200 0 0.85 6.0 Example 46 30000 250003000 25000 5000 200 0.70 4.0 Example 47 30000 25000 3000 25000 5000 2000.85 5.0 Example 48 30000 7000 1000 25000 5000 0 0.70 5.0 Example 4930000 7000 1000 25000 5000 0 0.85 6.0 Example 50 20000 16000 2000 100002000 100 0.70 4.0 Example 51 20000 16000 2000 10000 2000 100 0.85 5.0Example 52 30000 25000 3000 25000 5000 200 0.50 0.5 Example 53 1000025000 3000 25000 5000 200 0.50 0.5 Example 54 30000 25000 3000 1000 5000200 0.50 0.5

TABLE 6-2 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or Vertical more and 50 more and 100 101 nm more and 50 moreand 100 101 nm squareness SNR nm or less nm or less or more nm or lessnm or less or more ratio (dB) Comparative 8000 30000 1000 0 7000 2000.50 0.0 Example 19 Comparative 20000 16000 5000 600 2000 100 0.50 0.0Example 20 Comparative 32000 16000 500 10000 2000 280 0.50 0.0 Example21 Comparative 20000 16000 5000 10000 2000 280 0.50 0.0 Example 22Comparative 32000 16000 500 600 2000 450 0.50 0.0 Example 23 Comparative32000 16000 2000 0 7000 240 0.50 0.0 Example 24 Comparative 20000 300002000 0 7000 240 0.50 0.0 Example 25 Comparative 20000 30000 5000 0 7000240 0.50 0.0 Example 26 Comparative 8000 16000 2000 0 2000 80 0.50 0.0Example 27 Comparative 32000 5000 2000 0 2000 80 0.50 0.0 Example 28Comparative 32000 16000 5000 0 2000 80 0.50 0.0 Example 29 Comparative20000 5000 2000 0 7000 240 0.50 0.0 Example 30 Comparative 8000 300001000 0 7000 200 0.65 0.5 Example 31 Comparative 32000 16000 500 600 2000450 0.65 0.5 Example 32 Comparative 20000 5000 2000 0 7000 240 0.65 0.5Example 33 Comparative 800 30000 1000 0 7000 200 0.85 1.0 Example 34Comparative 8000 30000 1000 0 7000 200 0.50 1.0 Example 35 Comparative8000 30000 1000 0 7000 200 0.65 1.3 Example 36 Comparative 8000 300001000 0 7000 200 0.85 1.5 Example 37

From the results shown in Table 6, it can be confirmed that the use of amagnetic tape in which the number distribution A satisfies the above (1)to (3), the number distribution B satisfies the above (4) to (6), andthe vertical squareness ratio is 0.65 or more and 1.00 or less, and arecording head comprising a recording element provided with an alloylayer containing Co and Fe at the magnetic poles on both sides incombination with each other (Examples 24 to 51) is effective inimproving the electromagnetic conversion characteristics.

Examples 55 to 92 and Comparative Examples 38 to 54

A magnetic tape was manufactured in the same manner as in Example 1except that various items were changed as shown in Table 7, and theelectromagnetic conversion characteristics (SNR) of the manufacturedmagnetic tape were evaluated by the following method.

In Table 7, the vertical orientation treatment was not performed forExamples and Comparative Examples described as “OT” in the column of“magnetic field intensity during vertical orientation”.

Evaluation Method of Electromagnetic Conversion Characteristics

As the recording head, a recording head was used comprising a recordingelement having the same configuration (that is, a configuration in whicha layer made of an alloy containing Co and Fe is provided on themagnetic poles on both sides) as the recording element used in Example24 and the like except that the write gap length is the value shown inTable 7. Recording and reproduction were performed in the same manner asin Example 24, except for this point. The reproduction output duringreproduction was measured, and the SNR was obtained as asignal-to-noise-ratio (ratio between the reproduction output and noise).The SNR was calculated as a relative value where the SNR measured forComparative Example 38 was 0.0 dB. The evaluation results are shown inTable 8 (Table 8-1 and Table 8-2).

The vertical coercive force shown in Table 8 is a value obtained foreach magnetic tape by the method described above using a vibratingsample magnetometer (manufactured by Toei Industry Co., Ltd.).

The number distribution A and the number distribution B shown in Table 8were obtained by the same method as in Example 1 and the like.

TABLE 7 Magnetic field Recording intensity during element write Abrasiveliquid Filler liquid vertical gap length A B C D E F G orientation (nm)Example 55 6.0 parts 2.5 parts 20.0 parts 0.6 parts 0.8 parts 0.3 parts0.0 parts 0.3 T 120 Example 56 2.0 parts 2.5 parts 20.0 parts 0.6 parts5.0 parts 0.3 parts 0.0 parts 0.3 T 120 Example 57 6.0 parts 2.5 parts20.0 parts 0.0 parts 5.0 parts 0.3 parts 0.0 parts 0.3 T 120 Example 586.0 parts 0.7 parts 20.0 parts 0.6 parts 0.2 parts 0.3 parts 0.0 parts0.3 T 120 Example 59 6.0 parts 2.5 parts 6.7 parts 0.0 parts 0.2 parts0.3 parts 0.0 parts 0.3 T 120 Example 60 6.0 parts 0.7 parts 20.0 parts0.6 parts 0.2 parts 0.0 parts 0.0 parts 0.3 T 120 Example 61 6.0 parts0.7 parts 6.7 parts 0.6 parts 5.0 parts 0.0 parts 0.0 parts 0.3 T 120Example 62 4.0 parts 1.6 parts 13.3 parts 0.6 parts 5.0 parts 0.0 parts0.0 parts 0.3 T 120 Example 63 6.0 parts 2.5 parts 6.7 parts 0.3 parts2.0 parts 0.1 parts 0.0 parts 0.3 T 120 Example 64 4.0 parts 1.6 parts13.3 parts 0.3 parts 2.0 parts 0.1 parts 0.0 parts 0.3 T 120 Example 654.0 parts 0.7 parts 13.3 parts 0.0 parts 0.2 parts 0.1 parts 0.0 parts0.3 T 120 Example 66 6.0 parts 1.6 parts 6.7 parts 0.0 parts 2.0 parts0.3 pails 0.0 parts 0.3 T 120 Example 67 2.0 parts 2.5 parts 20.0 parts0.0 parts 0.2 parts 0.3 parts 0.0 parts 0.3 T 120 Example 68 2.0 parts0.7 parts 6.7 parts 0.6 parts 5.0 parts 0.3 parts 0.0 parts 0.3 T 120Example 69 6.0 parts 2.5 parts 20.0 parts 0.0 parts 0.2 parts 0.0 parts0.0 parts 0.3 T 120 Example 70 2.0 parts 0.7 parts 6.7 parts 0.6 parts0.2 parts 0.3 parts 0.0 parts 0.3 T 120 Example 71 6.0 parts 0.7 parts20.0 parts 0.0 parts 0.2 parts 0.0 parts 0.0 parts 0.3 T 120 Example 726.0 parts 0.7 parts 6.7 parts 0.6 parts 0.2 parts 0.0 parts 0.0 parts0.3 T 120 Example 73 2.0 parts 0.7 parts 20.0 parts 0.0 parts 0.2 parts0.3 parts 0.0 parts 0.3 T 120 Example 74 0.6 parts 0.1 parts 2.0 parts0.2 parts 0.1 parts 0.0 parts 0.0 parts 0.3 T 120 Example 75 0.6 parts0.1 parts 2.0 parts 0.2 parts 0.1 parts 0.0 parts 0.0 parts 0.3 T 100Example 76 0.6 parts 0.1 parts 2.0 parts 0.2 parts 0.1 parts 0.0 parts0.0 parts 0.3 T 80 Example 77 0.6 parts 0.1 parts 2.0 parts 0.2 parts0.1 parts 0.0 parts 0.0 parts 0.5 T 120 Example 78 0.6 parts 0.1 parts2.0 parts 0.2 parts 0.1 parts 0.0 parts 0.0 parts 0.8 T 120 Example 790.6 parts 0.1 parts 2.0 parts 0.2 parts 0.1 parts 0.0 parts 0.0 parts0.4 T 120 Example 80 2.8 parts 0.9 parts 6.0 parts 0.5 parts 0.3 parts0.2 parts 0.0 parts 0.5 T 120 Example 81 2.8 parts 0.9 parts 6.0 parts0.5 parts 0.3 parts 0.2 parts 0.0 parts 0.8 T 120 Example 82 6.0 parts0.7 parts 6.7 parts 0.6 parts 5.0 parts 0.0 parts 0.0 parts 0.5 T 120Example 83 6.0 parts 0.7 parts 6.7 parts 0.6 parts 5.0 parts 0.0 parts0.0 parts 0.8 T 120 Example 84 1.6 parts 0.5 parts 4.0 parts 0.3 parts1.0 part 0.1 parts 0.0 parts 0.5 T 120 Example 85 1.6 parts 0.5 parts4.0 parts 0.3 pails 1.0 part 0.1 parts 0.0 parts 0.8 T 120 Example 866.0 parts 0.7 parts 6.7 parts 0.6 parts 5.0 parts 0.0 parts 0.0 parts0.8 T 100 Example 87 6.0 parts 0.7 parts 6.7 parts 0.6 parts 5.0 parts0.0 parts 0.0 parts 0.8 T 80 Comparative 1.6 parts 3.0 parts 6.7 parts0.0 parts 7.0 parts 0.3 parts 0.0 parts 0 T 150 Example 38 Comparative4.0 parts 1.6 parts 33.3 parts 0.0 parts 2.0 parts 0.1 parts 0.0 parts 0T 150 Example 39 Comparative 6.4 parts 1.6 parts 3.3 parts 0.3 parts 2.0parts 0.4 parts 0.0 parts 0 T 150 Example 40 Comparative 4.0 parts 1.6parts 33.3 parts 0.3 parts 2.0 parts 0.4 parts 0.0 parts 0 T 150 Example41 Comparative 6.4 parts 1.6 parts 3.3 parts 0.0 parts 2.0 parts 0.6parts 0.0 parts 0 T 150 Example 42 Comparative 6.4 parts 1.6 parts 13.3parts 0.0 parts 0.0 parts 0.0 parts 3.0 parts 0 T 150 Example 43Comparative 4.0 parts 3.0 parts 13.3 parts 0.0 parts 0.0 parts 0.0 parts3.0 parts 0 T 150 Example 44 Comparative 4.0 parts 3.0 parts 33.3 parts0.0 parts 0.0 parts 0.0 parts 3.0 parts 0 T 150 Example 45 Comparative1.6 parts 1.6 parts 13.3 parts 0.0 parts 0.0 parts 0.0 parts 1.0 part 0T 150 Example 46 Comparative 6.4 parts 0.5 parts 13.3 parts 0.0 parts0.0 parts 0.0 parts 1.0 part 0 T 150 Example 47 Comparative 6.4 parts1.6 parts 33.3 parts 0.0 parts 0.0 parts 0.0 parts 1.0 part 0 T 150Example 48 Comparative 4.0 parts 0.5 parts 13.3 parts 0.0 parts 0.0parts 0.0 parts 3.0 parts 0 T 150 Example 49 Comparative 1.6 parts 3.0parts 6.7 parts 0.0 parts 7.0 parts 0.3 parts 0.0 parts 0.3 T 120Example 50 Comparative 6.4 parts 1.6 parts 3.3 parts 0.3 parts 2.0 parts0.4 parts 0.0 parts 0.5 T 120 Example 51 Comparative 1.6 parts 3.0 parts6.7 parts 0.0 parts 0.0 parts 0.0 parts 2.5 parts 0.8 T 120 Example 52Comparative 1.6 parts 3.0 parts 6.7 parts 0.0 parts 7.0 parts 0.3 parts0.0 parts 0.8 T 100 Example 53 Comparative 2.0 parts 2.5 parts 20.0parts 0.6 parts 5.0 parts 0.3 parts 0.0 parts 0 T 100 Example 54 Example88 6.0 parts 2.5 parts 20.0 parts 0.0 parts 5.0 parts 0.3 parts 0.0parts 0 T 100 Example 89 6.0 parts 0.7 parts 20.0 parts 0.6 parts 0.2parts 0.3 parts 0.0 parts 1.0 T 100 Example 90 2.0 parts 2.5 parts 20.0parts 0.6 parts 5.0 parts 0.3 parts 0.0 parts 1.0 T 120 Example 91 6.0parts 2.5 parts 20.0 parts 0.0 parts 5.0 parts 0.3 parts 0.0 parts 1.0 T120 Example 92 6.0 parts 0.7 parts 20.0 parts 0.6 parts 0.2 parts 0.3parts 0.0 parts 1.0 T 120

TABLE 8-1 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or Vertical more and 50 more and 100 101 nm more and 50 moreand 100 101 nm coercive SNR nm or less nm or less or more nm or less nmor less or more force (Oe) (dB) Example 55 30000 25000 3000 25000 5000200 2500 3.0 Example 56 10000 25000 3000 25000 5000 200 2500 3.0 Example57 30000 25000 3000 1000 5000 200 2500 3.0 Example 58 30000 7000 300025000 200 200 2500 3.0 Example 59 30000 25000 1000 1000 200 200 2500 3.0Example 60 30000 7000 3000 25000 200 0 2500 3.5 Example 61 30000 70001000 25000 5000 0 2500 3.5 Example 62 20000 16000 2000 25000 5000 0 25003.5 Example 63 30000 25000 1000 10000 2000 100 2500 3.0 Example 64 2000016000 2000 10000 2000 100 2500 3.0 Example 65 20000 7000 2000 1000 200100 2500 3.0 Example 66 30000 16000 1000 1000 2000 200 2500 3.0 Example67 10000 25000 3000 1000 200 200 2500 3.0 Example 68 10000 7000 100025000 5000 200 2500 3.0 Example 69 30000 25000 3000 1000 200 0 2500 3.5Example 70 10000 7000 1000 25000 200 200 2500 3.0 Example 71 30000 70003000 1000 200 0 2500 3.5 Example 72 30000 7000 1000 25000 200 0 2500 3.5Example 73 10000 7000 3000 1000 200 200 2500 3.0 Example 74 10000 70001000 1000 200 0 2500 3.5 Example 75 10000 7000 1000 1000 200 0 2500 5.0Example 76 10000 7000 1000 1000 200 0 2500 6.0 Example 77 10000 70001000 1000 200 0 3200 5.0 Example 78 10000 7000 1000 1000 200 0 3500 6.0Example 79 10000 7000 1000 1000 200 0 2800 4.5 Example 80 30000 250003000 25000 5000 200 3200 4.0 Example 81 30000 25000 3000 25000 5000 2003500 5.0 Example 82 30000 7000 1000 25000 5000 0 3200 5.0 Example 8330000 7000 1000 25000 5000 0 3500 6.0 Example 84 20000 16000 2000 100002000 100 3200 4.0 Example 85 20000 16000 2000 10000 2000 100 3500 5.0Example 86 30000 7000 1000 25000 5000 0 3500 7.0 Example 87 30000 70001000 25000 5000 0 3500 8.0

TABLE 8-2 Number distribution A Number distribution B 1 nm or 51 nm or 1nm or 51 nm or Vertical more and 50 more and 100 101 nm more and 50 moreand 100 101 nm coercive SNR nm or less nm or less or more nm or less nmor less or more force (Oe) (dB) Comparative 8000 30000 1000 0 7000 2002000 0.0 Example 38 Comparative 20000 16000 5000 600 2000 100 2000 0.0Example 39 Comparative 32000 16000 500 10000 2000 280 2000 0.0 Example40 Comparative 20000 16000 5000 10000 2000 280 2000 0.0 Example 41Comparative 32000 16000 500 600 2000 450 2000 0.0 Example 42 Comparative32000 16000 2000 0 7000 240 2000 0.0 Example 43 Comparative 20000 300002000 0 7000 240 2000 0.0 Example 44 Comparative 20000 30000 5000 0 7000240 2000 0.0 Example 45 Comparative 8000 16000 2000 0 2000 80 2000 0.0Example 46 Comparative 32000 5000 2000 0 2000 80 2000 0.0 Example 47Comparative 32000 16000 5000 0 2000 80 2000 0.0 Example 48 Comparative20000 5000 2000 0 7000 240 2000 0.0 Example 49 Comparative 8000 300001000 0 7000 200 2500 0.5 Examole 50 Comparative 32000 16000 500 100002000 280 3200 0.5 Example 51 Comparative 8000 30000 1000 0 7000 200 35001.0 Example 52 Comparative 8000 30000 1000 0 7000 200 3500 1.0 Example53 Comparative 10000 25000 3000 25000 5000 200 2000 1.0 Example 54Example 88 30000 25000 3000 1000 5000 200 2000 1.0 Example 89 30000 70003000 25000 200 200 2000 1.5 Example 90 10000 25000 3000 25000 5000 2003600 1.5 Example 91 30000 25000 3000 1000 5000 200 3600 0.5 Example 9230000 7000 3000 25000 200 200 3600 0.5

From the results shown in Table 8, it can be confirmed that the use of amagnetic tape in which the number distribution A satisfies the above (1)to (3), the number distribution B satisfies the above (4) to (6), andthe vertical coercive force is 2,500 Oe or more and 3,500 Oe or less,and a recording head comprising a recording element having a write gaplength of 120 nm or less in combination with each other (Examples 55 to87) is effective in improving the electromagnetic conversioncharacteristics.

An aspect of the present invention is useful in the technical field of amagnetic recording medium used as an archive recording medium. Further,an aspect of the present invention is useful in the technical field of amagnetic recording medium for high density recording.

What is claimed is:
 1. A magnetic recording medium comprising: anon-magnetic support; and a magnetic layer including ferromagneticpowder, wherein a number distribution A of a plurality of brightregions, based on equivalent circle diameters thereof, in a binarizedimage of a secondary electron image obtained by imaging a surface of themagnetic layer by a scanning electron microscope at an accelerationvoltage of 5 kV satisfies the following (1) to (3): (1) bright regionshaving an equivalent circle diameter of 1 nm or more and 50 nm or lessare 10,000 or more and 30,000 or less; (2) bright regions having anequivalent circle diameter of 51 nm or more and 100 nm or less are 7,000or more and 25,000 or less; and (3) bright regions having an equivalentcircle diameter of 101 nm or more are 1,000 or more and 3,000 or less,and a number distribution B of a plurality of dark regions, based onequivalent circle diameters thereof, in a binarized image of a secondaryelectron image obtained by imaging a surface of the magnetic layer by ascanning electron microscope at an acceleration voltage of 2 kVsatisfies the following (4) to (6): (4) dark regions having anequivalent circle diameter of 1 nm or more and 50 nm or less are 1,000or more and 25,000 or less; (5) dark regions having an equivalent circlediameter of 51 nm or more and 100 nm or less are 200 or more and 5,000or less; and (6) dark regions having an equivalent circle diameter of101 nm or more are 0 or more and 200 or less.
 2. The magnetic recordingmedium according to claim 1, wherein a total thickness of the magneticrecording medium is 5.3 μm or less.
 3. The magnetic recording mediumaccording to claim 1, further comprising: a non-magnetic layer includingnon-magnetic powder between the non-magnetic support and the magneticlayer.
 4. The magnetic recording medium according to claim 1, furthercomprising: a back coating layer including non-magnetic powder on asurface side of the non-magnetic support opposite to a surface sideprovided with the magnetic layer.
 5. The magnetic recording mediumaccording to claim 1, wherein the magnetic layer includes two or moretypes of non-magnetic powder.
 6. The magnetic recording medium accordingto claim 5, wherein the non-magnetic powder of the magnetic layerincludes alumina powder.
 7. The magnetic recording medium according toclaim 5, wherein the non-magnetic powder of the magnetic layer includescarbon black.
 8. The magnetic recording medium according to claim 1,wherein the ferromagnetic powder is hexagonal barium ferrite powder. 9.The magnetic recording medium according to claim 1, wherein theferromagnetic powder is hexagonal strontium ferrite powder.
 10. Themagnetic recording medium according to claim 1, wherein theferromagnetic powder is ε-iron oxide powder.
 11. The magnetic recordingmedium according to claim 1, wherein a vertical squareness ratio is 0.65or more and 1.00 or less.
 12. The magnetic recording medium according toclaim 1, wherein a vertical coercive force is 2,500 Oe or more and 3,500Oe or less.
 13. The magnetic recording medium according to claim 1,wherein the magnetic recording medium is a magnetic tape.
 14. A magneticrecording and reproducing apparatus comprising: the magnetic recordingmedium according to claim
 1. 15. The magnetic recording and reproducingapparatus according to claim 14, further comprising: a magnetic headthat has an inductive recording element having a first magnetic polethat generates a magnetic field and a second magnetic pole that isseparated from the first magnetic pole with a write gap therebetween,wherein the first magnetic pole has a layer made of an alloy containingCo and Fe as an outermost layer of a portion facing the second magneticpole with the write gap therebetween, and the second magnetic pole has alayer made of an alloy containing Co and Fe as an outermost layer of aportion facing the first magnetic pole with the write gap therebetween.16. The magnetic recording and reproducing apparatus according to claim14, further comprising: a magnetic head having an inductive recordingelement having a length of a write gap of 120 nm or less.
 17. A magnetictape cartridge comprising: the magnetic recording medium according toclaim
 13. 18. A magnetic tape cartridge group comprising: a plurality ofthe magnetic tape cartridges according to claim
 17. 19. The magnetictape cartridge group according to claim 18, wherein, in an environmentof an atmosphere temperature of 21° C. and a relative humidity of 50%, aslope α of a signal-to-noise-ratio with respect to the number of rolls,the slope α being obtained by performing a reproduction test of a totalof 200 rolls of the magnetic tape cartridges using a single magnetichead, is 0.5 dB/decade or less.